Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive force. The seventh lens have negative refractive force, wherein both surfaces thereof can be aspheric, and at least one surface thereof has an inflection point. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imagining quality for use in compact cameras.

BACKGROUND OF THE INVENTION

1. Technical Field

The present invention generally relates to an optical system, and moreparticularly to a compact optical image capturing system for anelectronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of the ordinaryphotographing camera is commonly selected from charge coupled device(CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor).Also, as advanced semiconductor manufacturing technology enables theminimization of the pixel size of the image sensing device, thedevelopment of the optical image capturing system towards the field ofhigh pixels. Therefore, the requirement for high imaging quality israpidly raised.

The conventional optical system of the portable electronic deviceusually has five or sixth lenses. However, the optical system is askedto take pictures in a dark environment, in other words, the opticalsystem is asked to have a large aperture. The conventional opticalsystem provides high optical performance as required.

It is an important issue to increase the quantity of light entering thelens. Also, the modern lens is also asked to have several characters,including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofseven-piece optical lenses (the convex or concave surface in thedisclosure denotes the geometrical shape of an image-side surface or anobject-side surface of each lens on an optical axis) to increase thequantity of incoming light of the optical image capturing system, and toimprove imaging quality for image formation, so as to be applied tominimized electronic products.

The term and its definition to the lens parameter in the embodiment ofthe present are shown as below for further reference.

The lens parameter related to a length or a height in the lens:

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens to the image-side surface of the seventh lens is denoted by InTL. Adistance from the first lens to the second lens is denoted by IN12(instance). A central thickness of the first lens of the optical imagecapturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing systemis denoted by NA1 (instance). A refractive index of the first lens isdenoted by Nd1 (instance).

The lens parameter related to a view angle of the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. For any surface of any lens, a maximum effective halfdiameter (EHD) is a perpendicular distance between an optical axis and acrossing point on the surface where the incident light with a maximumviewing angle of the system passing the very edge of the entrance pupil.For example, the maximum effective half diameter of the object-sidesurface of the first lens is denoted by EHD11, the maximum effectivehalf diameter of the image-side surface of the first lens is denoted byEHD12, the maximum effective half diameter of the object-side surface ofthe second lens is denoted by EHD21, the maximum effective half diameterof the image-side surface of the second lens is denoted by EHD22, and soon.

The lens parameter related to a depth of the lens shape:

A distance in parallel with the optical axis from a point where theoptical axis passes through to an end point of the maximum effectivesemi diameter on the object-side surface of the seventh lens is denotedby InRS71 (the depth of the maximum effective semi diameter). A distancein parallel with the optical axis from a point where the optical axispasses through to an end point of the maximum effective semi diameter onthe image-side surface of the seventh lens is denoted by InRS72 (thedepth of the maximum effective semi diameter). The depth of the maximumeffective semi diameter (sinkage) on the object-side surface or theimage-side surface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens,and the tangent point is tangent to a plane perpendicular to the opticalaxis and the tangent point cannot be a crossover point on the opticalaxis. Following the above description, a distance perpendicular to theoptical axis between a critical point C51 on the object-side surface ofthe fifth lens and the optical axis is HVT51 (instance), and a distanceperpendicular to the optical axis between a critical point C52 on theimage-side surface of the fifth lens and the optical axis is HVT52(instance). A distance perpendicular to the optical axis between acritical point C61 on the object-side surface of the sixth lens and theoptical axis is HVT61 (instance), and a distance perpendicular to theoptical axis between a critical point C62 on the image-side surface ofthe sixth lens and the optical axis is HVT62 (instance). A distanceperpendicular to the optical axis between a critical point on theobject-side or image-side surface of other lenses, such as the seventhlens, the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection pointIF711 which is nearest to the optical axis, and the sinkage value of theinflection point IF711 is denoted by SGI711 (instance). A distanceperpendicular to the optical axis between the inflection point IF711 andthe optical axis is HIF711 (instance). The image-side surface of theseventh lens has one inflection point IF721 which is nearest to theoptical axis, and the sinkage value of the inflection point IF721 isdenoted by SGI721 (instance). A distance perpendicular to the opticalaxis between the inflection point IF721 and the optical axis is HIF721(instance).

The object-side surface of the seventh lens has one inflection pointIF712 which is the second nearest to the optical axis, and the sinkagevalue of the inflection point IF712 is denoted by SGI712 (instance). Adistance perpendicular to the optical axis between the inflection pointIF712 and the optical axis is HIF712 (instance). The image-side surfaceof the seventh lens has one inflection point IF722 which is the secondnearest to the optical axis, and the sinkage value of the inflectionpoint IF722 is denoted by SGI722 (instance). A distance perpendicular tothe optical axis between the inflection point IF722 and the optical axisis HIF722 (instance).

The object-side surface of the seventh lens has one inflection pointIF713 which is the third nearest to the optical axis, and the sinkagevalue of the inflection point IF713 is denoted by SGI713 (instance). Adistance perpendicular to the optical axis between the inflection pointIF713 and the optical axis is HIF713 (instance). The image-side surfaceof the seventh lens has one inflection point IF723 which is the thirdnearest to the optical axis, and the sinkage value of the inflectionpoint IF723 is denoted by SGI723 (instance). A distance perpendicular tothe optical axis between the inflection point IF723 and the optical axisis HIF723 (instance).

The object-side surface of the seventh lens has one inflection pointIF714 which is the fourth nearest to the optical axis, and the sinkagevalue of the inflection point IF714 is denoted by SGI714 (instance). Adistance perpendicular to the optical axis between the inflection pointIF714 and the optical axis is HIF714 (instance). The image-side surfaceof the seventh lens has one inflection point IF724 which is the fourthnearest to the optical axis, and the sinkage value of the inflectionpoint IF724 is denoted by SGI724 (instance). A distance perpendicular tothe optical axis between the inflection point IF724 and the optical axisis HIF724 (instance).

An inflection point, a distance perpendicular to the optical axisbetween the inflection point and the optical axis, and a sinkage valuethereof on the object-side surface or image-side surface of other lensesis denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100% field. An offset of the spherical aberration is denoted by DFS.An offset of the coma aberration is denoted by DFC.

A modulation transfer function (MTF) graph of an optical image capturingsystem is used to test and evaluate the contrast and sharpness of thegenerated images. The vertical axis of the coordinate system of the MTFgraph represents the contrast transfer rate, of which the value isbetween 0 and 1, and the horizontal axis of the coordinate systemrepresents the spatial frequency, of which the unit is cycles/mm orlp/mm, i.e., line pairs per millimeter. Theoretically, a perfect opticalimage capturing system can present all detailed contrast and every lineof an object in an image. However, the contrast transfer rate of apractical optical image capturing system along a vertical axis thereofwould be less than 1. In addition, peripheral areas in an image wouldhave a poorer realistic effect than a center area thereof has. Forvisible spectrum, the values of MTF in the spatial frequency of 55cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of viewon an image plane are respectively denoted by MTFE0, MTFE3, and MTFE7;the values of MTF in the spatial frequency of 110 cycles/mm at theoptical axis, 0.3 field of view, and 0.7 field of view on an image planeare respectively denoted by MTFQ0, MTFQ3, and MTFQ7; the values of MTFin the spatial frequency of 220 cycles/mm at the optical axis, 0.3 fieldof view, and 0.7 field of view on an image plane are respectivelydenoted by MTFH0, MTFH3, and MTFH7; the values of MTF in the spatialfrequency of 440 cycles/mm at the optical axis, 0.3 field of view, and0.7 field of view on the image plane are respectively denoted by MTF0,MTF3, and MTF7. The three aforementioned fields of view respectivelyrepresent the center, the inner field of view, and the outer field ofview of a lens, and, therefore, can be used to evaluate the performanceof an optical image capturing system. If the optical image capturingsystem provided in the present invention corresponds to photosensitivecomponents which provide pixels having a size no large than 1.12micrometer, a quarter of the spatial frequency, a half of the spatialfrequency (half frequency), and the full spatial frequency (fullfrequency) of the MTF diagram are respectively at least 110 cycles/mm,220 cycles/mm and 440 cycles/mm.

If an optical image capturing system is required to be able also toimage for infrared spectrum, e.g., to be used in low-light environments,then the optical image capturing system should be workable inwavelengths of 850 nm or 800 nm. Since the main function for an opticalimage capturing system used in low-light environment is to distinguishthe shape of objects by light and shade, which does not require highresolution, it is appropriate to only use spatial frequency less than110 cycles/mm for evaluating the performance of optical image capturingsystem in the infrared spectrum. When the aforementioned wavelength of850 nm focuses on the image plane, the contrast transfer rates (i.e.,the values of MTF) in spatial frequency of 55 cycles/mm at the opticalaxis, 0.3 field of view, and 0.7 field of view on an image plane arerespectively denoted by MTFI0, MTFI3, and MTFI7. However, infraredwavelengths of 850 nm or 800 nm are far away from the wavelengths ofvisible light; it would be difficult to design an optical imagecapturing system capable of focusing visible and infrared light (i.e.,dual-mode) at the same time and achieving certain performance.

The present invention provides an optical image capturing system, whichis capable of focusing visible and infrared light (i.e., dual-mode) atthe same time and achieving certain performance, wherein the seventhlens thereof is provided with an inflection point at the object-sidesurface or at the image-side surface to adjust the incident angle ofeach view field and modify the ODT and the TDT. In addition, thesurfaces of the seventh lens are capable of modifying the optical pathto improve the imagining quality.

The optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens, asixth lens, a seventh lens, and an image plane in order along an opticalaxis from an object side to an image side. At least one lens among thefirst lens to the seventh lens is made of glass, and at least one lensamong the first lens to the seventh lens is made of plastic. The opticalimage capturing system satisfies:

1.0≦f/HEP≦10.0;0 deg<HAF≦150 and 0.2≦EIN/ETL<1;

where f1, f2, f3, f4, f5, f6, and f7 are respectively a focal length ofthe first lens to the seventh lens; f is a focal length of the opticalimage capturing system; HEP is an entrance pupil diameter of the opticalimage capturing system; HOS is a distance between the object-sidesurface of the first lens and the image plane; InTL is a distance fromthe object-side surface of the first lens to the image-side surface ofthe seventh lens on the optical axis; HAF is a half of the maximum fieldangle of the optical image capturing system; ETL is a distance inparallel with the optical axis between a coordinate point at a height of½ HEP on the object-side surface of the first lens and the image plane;EIN is a distance in parallel with the optical axis between thecoordinate point at the height of ½ HEP on the object-side surface ofthe first lens and a coordinate point at a height of ½ HEP on theimage-side surface of the seventh lens.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a sixth lens, a seventh lens, and an image plane, inorder along an optical axis from an object side to an image side. Thefirst lens is made of glass, and at least two lenses among the secondlens to the seventh lens are made of plastic. The optical imagecapturing system has a maximum height HOI for image formation on theimage plane. The object-side surface or the image-side surface of atleast one lens among the first lens to the seventh lens has at least aninflection point thereon. At least one lens among the second lens to theseventh lens has positive refractive power. The first lens has negativerefractive power. The second les has refractive power. The third lenshas refractive power. The fourth lens has refractive power. The fifthlens has refractive power. The sixth lens has refractive power. Theseventh lens has refractive power, and an object-side surface and animage-side surface thereof are both aspheric. The optical imagecapturing system satisfies:

1.0≦f/HEP≦10.0;0 deg<HAF≦150; and 0.2≦EIN/ETL<1;

where f1, f2, f3, f4, f5, f6, and f7 are respectively a focal length ofthe first lens to the seventh lens; f is a focal length of the opticalimage capturing system; HEP is an entrance pupil diameter of the opticalimage capturing system; HOS is a distance between the object-sidesurface of the first lens and the image plane; InTL is a distance fromthe object-side surface of the first lens to the image-side surface ofthe seventh lens on the optical axis; HAF is a half of the maximum fieldangle of the optical image capturing system; ETL is a distance inparallel with the optical axis between a coordinate point at a height of½ HEP on the object-side surface of the first lens and the image plane;EIN is a distance in parallel with the optical axis between thecoordinate point at the height of ½ HEP on the object-side surface ofthe first lens and a coordinate point at a height of ½ HEP on theimage-side surface of the seventh lens.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a sixth lens, a seventh lens, and an image plane, inorder along an optical axis from an object side to an image side. Thenumber of the lenses having refractive power in the optical imagecapturing system is seven. At least two lenses among the first lens tothe seventh lens are made of plastic, and the other five lenses are madeof glass. At least one lens among the second lens to the fourth lens haspositive refractive power. At least one lens among the fifth lens to theseventh lens has positive refractive power. The optical image capturingsystem has a maximum height HOI for image formation on the image plane.The object-side surface or the image-side surface of each of the atleast one lens among the first lens to the seventh lens has at least aninflection point thereon. The first lens has negative refractive power,and the second lens has refractive power. The third lens has refractivepower. The fourth lens has refractive power. The fifth lens hasrefractive power. The sixth lens has refractive power. The seventh lenshas refractive power. The optical image capturing system satisfies:

1.0≦f/HEP≦6.0;0 deg<HAF≦100 deg; and 0.2≦EIN/ETL<1;

where f1, f2, f3, f4, f5, f6, and f7 are respectively a focal length ofthe first lens to the seventh lens; f is a focal length of the opticalimage capturing system; HEP is an entrance pupil diameter of the opticalimage capturing system; HOS is a distance between a point on anobject-side surface, which face the object side, of the first lens wherethe optical axis passes through and a point on the image plane where theoptical axis passes through; InTL is a distance from the object-sidesurface of the first lens to the image-side surface of the seventh lenson the optical axis; HAF is a half of the maximum field angle of theoptical image capturing system; ETL is a distance in parallel with theoptical axis between a coordinate point at a height of ½ HEP on theobject-side surface of the first lens and the image plane; EIN is adistance in parallel with the optical axis between the coordinate pointat the height of ½ HEP on the object-side surface of the first lens anda coordinate point at a height of ½ HEP on the image-side surface of theseventh lens.

For any lens, the thickness at the height of a half of the entrancepupil diameter (HEP) particularly affects the ability of correctingaberration and differences between optical paths of light in differentfields of view of the common region of each field of view of lightwithin the covered range at the height of a half of the entrance pupildiameter (HEP). With greater thickness, the ability to correctaberration is better. However, the difficulty of manufacturing increasesas well. Therefore, the thickness at the height of a half of theentrance pupil diameter (HEP) of any lens has to be controlled. Theratio between the thickness (ETP) at the height of a half of theentrance pupil diameter (HEP) and the thickness (TP) of any lens on theoptical axis (i.e., ETP/TP) has to be particularly controlled. Forexample, the thickness at the height of a half of the entrance pupildiameter (HEP) of the first lens is denoted by ETP1, the thickness atthe height of a half of the entrance pupil diameter (HEP) of the secondlens is denoted by ETP2, and the thickness at the height of a half ofthe entrance pupil diameter (HEP) of any other lens in the optical imagecapturing system is denoted in the same manner. The optical imagecapturing system of the present invention satisfies:

0.3≦SETP/EIN<1;

where SETP is the sum of the aforementioned ETP1 to ETP5.

In order to enhance the ability of correcting aberration and to lowerthe difficulty of manufacturing at the same time, the ratio between thethickness (ETP) at the height of a half of the entrance pupil diameter(HEP) and the thickness (TP) of any lens on the optical axis (i.e.,ETP/TP) has to be particularly controlled. For example, the thickness atthe height of a half of the entrance pupil diameter (HEP) of the firstlens is denoted by ETP1, the thickness of the first lens on the opticalaxis is TP1, and the ratio between these two parameters is ETP1/TP1; thethickness at the height of a half of the entrance pupil diameter (HEP)of the first lens is denoted by ETP2, the thickness of the second lenson the optical axis is TP2, and the ratio between these two parametersis ETP2/TP2. The ratio between the thickness at the height of a half ofthe entrance pupil diameter (HEP) and the thickness of any other lens inthe optical image capturing system is denoted in the same manner. Theoptical image capturing system of the present invention satisfies:

0.2≦ETP/TP≦3.

The horizontal distance between two neighboring lenses at the height ofa half of the entrance pupil diameter (HEP) is denoted by ED, whereinthe aforementioned horizontal distance (ED) is parallel to the opticalaxis of the optical image capturing system, and particularly affects theability of correcting aberration and differences between optical pathsof light in different fields of view of the common region of each fieldof view of light at the height of a half of the entrance pupil diameter(HEP). With longer distance, the ability to correct aberration ispotential to be better. However, the difficulty of manufacturingincreases, and the feasibility of “slightly shorten” the length of theoptical image capturing system is limited as well. Therefore, thehorizontal distance (ED) between two specific neighboring lenses at theheight of a half of the entrance pupil diameter (HEP) has to becontrolled.

In order to enhance the ability of correcting aberration and to lowerthe difficulty of “slightly shorten” the length of the optical imagecapturing system at the same time, the ratio between the horizontaldistance (ED) between two neighboring lenses at the height of a half ofthe entrance pupil diameter (HEP) and the parallel distance (IN) betweenthese two neighboring lens on the optical axis (i.e., ED/IN) has to beparticularly controlled. For example, the horizontal distance betweenthe first lens and the second lens at the height of a half of theentrance pupil diameter (HEP) is denoted by ED12, the horizontaldistance between the first lens and the second lens on the optical axisis denoted by IN12, and the ratio between these two parameters isED12/IN12; the horizontal distance between the second lens and the thirdlens at the height of a half of the entrance pupil diameter (HEP) isdenoted by ED23, the horizontal distance between the second lens and thethird lens on the optical axis is denoted by IN23, and the ratio betweenthese two parameters is ED23/IN23. The ratio between the horizontaldistance between any two neighboring lenses at the height of a half ofthe entrance pupil diameter (HEP) and the horizontal distance betweenthese two neighboring lenses on the optical axis is denoted in the samemanner.

The horizontal distance in parallel with the optical axis between acoordinate point at the height of ½ HEP on the image-side surface of theseventh lens and image surface is denoted by EBL. The horizontaldistance in parallel with the optical axis between the point on theimage-side surface of the seventh lens where the optical axis passesthrough and the image plane is denoted by BL. To enhance the ability tocorrect aberration and to preserve more space for other opticalcomponents, the optical image capturing system of the present inventioncan satisfy 0.2≦EBL/BL≦1.1. The optical image capturing system canfurther include a filtering component, which is provided between theseventh lens and the image plane, wherein the horizontal distance inparallel with the optical axis between the coordinate point at theheight of ½ HEP on the image-side surface of the seventh lens and thefiltering component is denoted by EIR, and the horizontal distance inparallel with the optical axis between the point on the image-sidesurface of the seventh lens where the optical axis passes through andthe filtering component is denoted by PIR. The optical image capturingsystem of the present invention can satisfy 0.1≦EIR/PIR≦1.

In an embodiment, a height of the optical image capturing system (HOS)can be reduced while |f1|>|f7|.

In an embodiment, when the lenses satisfy |f2|+|f3|+|f4|+|f5|+|f6| and|f1|×|f7|, at least one lens among the second to the sixth lenses couldhave weak positive refractive power or weak negative refractive power.Herein the weak refractive power means the absolute value of the focallength of one specific lens is greater than 10. When at least one lensamong the second to the sixth lenses has weak positive refractive power,it may share the positive refractive power of the first lens, and on thecontrary, when at least one lens among the second to the sixth lenseshas weak negative refractive power, it may fine tune and correct theaberration of the system.

In an embodiment, the seventh lens could have negative refractive power,and an image-side surface thereof is concave, it may reduce back focallength and size. Besides, the seventh lens can have at least aninflection point on at least a surface thereof, which may reduce anincident angle of the light of an off-axis field of view and correct theaberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to thefollowing detailed description of some illustrative embodiments inconjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the presentinvention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the first embodiment of thepresent application;

FIG. 1C shows a feature map of modulation transformation of the opticalimage capturing system of the first embodiment of the presentapplication in visible spectrum;

FIG. 2A is a schematic diagram of a second embodiment of the presentinvention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the second embodiment of thepresent application;

FIG. 2C shows a feature map of modulation transformation of the opticalimage capturing system of the second embodiment of the presentapplication in visible spectrum;

FIG. 3A is a schematic diagram of a third embodiment of the presentinvention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the third embodiment of thepresent application;

FIG. 3C shows a feature map of modulation transformation of the opticalimage capturing system of the third embodiment of the presentapplication in visible spectrum;

FIG. 4A is a schematic diagram of a fourth embodiment of the presentinvention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fourth embodiment of thepresent application;

FIG. 4C shows a feature map of modulation transformation of the opticalimage capturing system of the fourth embodiment in visible spectrum;

FIG. 5A is a schematic diagram of a fifth embodiment of the presentinvention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fifth embodiment of thepresent application;

FIG. 5C shows a feature map of modulation transformation of the opticalimage capturing system of the fifth embodiment of the presentapplication in visible spectrum;

FIG. 6A is a schematic diagram of a sixth embodiment of the presentinvention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the sixth embodiment of thepresent application;

FIG. 6C shows a feature map of modulation transformation of the opticalimage capturing system of the sixth embodiment of the presentapplication in visible spectrum;

FIG. 7A is a schematic diagram of a seventh embodiment of the presentinvention;

FIG. 7B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the seventh embodiment of thepresent application;

FIG. 7C shows a feature map of modulation transformation of the opticalimage capturing system of the seventh embodiment of the presentapplication in visible spectrum;

FIG. 8A is a schematic diagram of a eighth embodiment of the presentinvention;

FIG. 8B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the eighth embodiment of thepresent application; and

FIG. 8C shows a feature map of modulation transformation of the opticalimage capturing system of the eighth embodiment of the presentapplication in visible spectrum.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens, asixth lens, a seventh lens, and an image plane from an object side to animage side. The optical image capturing system further is provided withan image sensor at an image plane. Image heights in the followingembodiments are all almost 3.91 mm.

The optical image capturing system can work in three wavelengths,including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the mainreference wavelength and is the reference wavelength for obtaining thetechnical characters. The optical image capturing system can also workin five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650nm wherein 555 nm is the main reference wavelength, and is the referencewavelength for obtaining the technical characters.

The optical image capturing system of the present invention satisfies0.5≦ΣPPR/|ΣNPR|≦15, and a preferable range is 1≦ΣPPR/|ΣNPR|≦3.0, wherePPR is a ratio of the focal length f of the optical image capturingsystem to a focal length fp of each of lenses with positive refractivepower; NPR is a ratio of the focal length f of the optical imagecapturing system to a focal length fn of each of lenses with negativerefractive power; ΣPPR is a sum of the PPRs of each positive lens; andΣNPR is a sum of the NPRs of each negative lens. It is helpful forcontrol of an entire refractive power and an entire length of theoptical image capturing system.

The image sensor is provided on the image plane. The optical imagecapturing system of the present invention satisfies HOS/HOI≦10 and0.5≦HOS/f≦10, and a preferable range is 1≦HOS/HOI≦5 and 1≦HOS/f≦7, whereHOI is a half of a diagonal of an effective sensing area of the imagesensor, i.e., the maximum image height, and HOS is a height of theoptical image capturing system, i.e. a distance on the optical axisbetween the object-side surface of the first lens and the image plane.It is helpful for reduction of the size of the system for used incompact cameras.

The optical image capturing system of the present invention further isprovided with an aperture to increase image quality.

In the optical image capturing system of the present invention, theaperture could be a front aperture or a middle aperture, wherein thefront aperture is provided between the object and the first lens, andthe middle is provided between the first lens and the image plane. Thefront aperture provides a long distance between an exit pupil of thesystem and the image plane, which allows more elements to be installed.The middle could enlarge a view angle of view of the system and increasethe efficiency of the image sensor. The optical image capturing systemsatisfies 0.2≦InS/HOS≦1.1, where InS is a distance between the apertureand the image-side surface of the sixth lens. It is helpful for sizereduction and wide angle.

The optical image capturing system of the present invention satisfies0.1≦ΣTP/InTL≦0.9, where InTL is a distance between the object-sidesurface of the first lens and the image-side surface of the seventhlens, and ΣTP is a sum of central thicknesses of the lenses on theoptical axis. It is helpful for the contrast of image and yield rate ofmanufacture and provides a suitable back focal length for installationof other elements.

The optical image capturing system of the present invention satisfies0.001≦|R1/R2|≦20, and a preferable range is 0.01≦|R1/R2|≦10, where R1 isa radius of curvature of the object-side surface of the first lens, andR2 is a radius of curvature of the image-side surface of the first lens.It provides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies−7<(R13−R14)/(R13+R14)<50, where R13 is a radius of curvature of theobject-side surface of the seventh lens, and R14 is a radius ofcurvature of the image-side surface of the seventh lens. It may modifythe astigmatic field curvature.

The optical image capturing system of the present invention satisfiesIN12/f≦3.0, where IN12 is a distance on the optical axis between thefirst lens and the second lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfiesIN67/f≦0.8, where IN67 is a distance on the optical axis between thesixth lens and the seventh lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfies0.1≦(TP1+IN12)/TP2≦10, where TP1 is a central thickness of the firstlens on the optical axis, and TP2 is a central thickness of the secondlens on the optical axis. It may control the sensitivity of manufactureof the system and improve the performance.

The optical image capturing system of the present invention satisfies0.1≦(TP7+IN67)/TP6≦10, where TP6 is a central thickness of the sixthlens on the optical axis, TP7 is a central thickness of the seventh lenson the optical axis, and IN67 is a distance between the sixth lens andthe seventh lens. It may control the sensitivity of manufacture of thesystem and improve the performance.

The optical image capturing system of the present invention satisfies0.1≦TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the thirdlens on the optical axis, TP4 is a central thickness of the fourth lenson the optical axis, TP5 is a central thickness of the fifth lens on theoptical axis, IN34 is a distance on the optical axis between the thirdlens and the fourth lens, IN45 is a distance on the optical axis betweenthe fourth lens and the fifth lens, and InTL is a distance between theobject-side surface of the first lens and the image-side surface of theseventh lens. It may fine tune and correct the aberration of theincident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≦HVT71≦3 mm; 0mm<HVT72≦6 mm; 0≦HVT71/HVT72; 0 mm≦|SGC71|≦0.5 mm; 0 mm<|SGC72|≦2 mm;and 0<|SGC72|/(|SGC72|+TP7)≦0.9, where HVT71 a distance perpendicular tothe optical axis between the critical point C71 on the object-sidesurface of the seventh lens and the optical axis; HVT72 a distanceperpendicular to the optical axis between the critical point C72 on theimage-side surface of the seventh lens and the optical axis; SGC71 is adistance in parallel with the optical axis between an point on theobject-side surface of the seventh lens where the optical axis passesthrough and the critical point C71; SGC72 is a distance in parallel withthe optical axis between an point on the image-side surface of theseventh lens where the optical axis passes through and the criticalpoint C72. It is helpful to correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≦HVT72/HOI≦0.9, andpreferably satisfies 0.3≦HVT72/HOI≦0.8. It may help to correct theperipheral aberration.

The optical image capturing system satisfies 0≦HVT72/HOS≦0.5, andpreferably satisfies 0.2≦HVT72/HOS≦0.45. It may help to correct theperipheral aberration.

The optical image capturing system of the present invention satisfies0<SGI711/(SGI711+TP7)≦0.9; 0<SGI721/(SGI721+TP7)≦0.9, and it ispreferable to satisfy 0.1≦SGI711/(SGI711+TP7)≦0.6;0.1≦SGI721/(SGI721+TP7)≦0.6, where SGI711 is a displacement in parallelwith the optical axis, from a point on the object-side surface of theseventh lens, through which the optical axis passes, to the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, and SGI721 is a displacement in parallel with the optical axis,from a point on the image-side surface of the seventh lens, throughwhich the optical axis passes, to the inflection point on the image-sidesurface, which is the closest to the optical axis.

The optical image capturing system of the present invention satisfies0<SGI712/(SGI712+TP7)≦0.9; 0<SGI722/(SGI722+TP7)≦0.9, and it ispreferable to satisfy 0.1≦SGI712/(SGI712+TP7)≦0.6;0.1≦SGI722/(SGI722+TP7)≦0.6, where SGI712 is a displacement in parallelwith the optical axis, from a point on the object-side surface of theseventh lens, through which the optical axis passes, to the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, and SGI722 is a displacement in parallel with the opticalaxis, from a point on the image-side surface of the seventh lens,through which the optical axis passes, to the inflection point on theimage-side surface, which is the second closest to the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≦|HIF711|≦5 mm; 0.001 mm≦|HIF721|≦5 mm, and it is preferable tosatisfy 0.1 mm≦|HIF711|≦3.5 mm; 1.5 mm≦|HIF721|≦3.5 mm, where HIF711 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is theclosest to the optical axis, and the optical axis; HIF721 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the seventh lens, which is the closest to theoptical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≦|HIF712|≦5 mm; 0.001 mm<|HIF722|≦5 mm, and it is preferable tosatisfy 0.1 mm≦|HIF722|≦3.5 mm; 0.1 mm≦|HIF712|≦3.5 mm, where HIF712 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is thesecond closest to the optical axis, and the optical axis; HIF722 is adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the seventh lens, which is the secondclosest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≦|HIF713|≦5 mm; 0.001 mm≦|HIF723|≦5 mm, and it is preferable tosatisfy 0.1 mm≦|HIF723|≦3.5 mm; 0.1 mm≦|HIF713|≦3.5 mm, where HIF713 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is the thirdclosest to the optical axis, and the optical axis; HIF723 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the seventh lens, which is the third closest tothe optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≦|HIF714|≦5 mm; 0.001 mm≦|HIF724|≦5 mm, and it is preferable tosatisfy 0.1 mm≦|HIF724|≦3.5 mm; 0.1 mm≦|HIF714|≦3.5 mm, where HIF714 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is thefourth closest to the optical axis, and the optical axis; HIF724 is adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the seventh lens, which is the fourthclosest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of lowAbbe number are arranged in an interlaced arrangement that could behelpful for correction of aberration of the system.

An equation of aspheric surface is

z=ch ²/[1+[1(k+1)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .  (1)

where z is a depression of the aspheric surface; k is conic constant; cis reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14,A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made ofplastic or glass. The plastic lenses may reduce the weight and lower thecost of the system, and the glass lenses may control the thermal effectand enlarge the space for arrangement of the refractive power of thesystem. In addition, the opposite surfaces (object-side surface andimage-side surface) of the first to the seventh lenses could be asphericthat can obtain more control parameters to reduce aberration. The numberof aspheric glass lenses could be less than the conventional sphericalglass lenses, which is helpful for reduction of the height of thesystem.

When the lens has a convex surface, which means that the surface isconvex around a position, through which the optical axis passes, andwhen the lens has a concave surface, which means that the surface isconcave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could beapplied in a dynamic focusing optical system. It is superior in thecorrection of aberration and high imaging quality so that it could beallied in lots of fields.

The optical image capturing system of the present invention couldfurther include a driving module to meet different demands, wherein thedriving module can be coupled with the lenses to move the lenses. Thedriving module can be a voice coil motor (VCM), which is used to movethe lens for focusing, or can be an optical image stabilization (OIS)component, which is used to lower the possibility of having the problemof image blurring which is caused by subtle movements of the lens whileshooting.

To meet different requirements, at least one lens among the first lensto the seventh lens of the optical image capturing system of the presentinvention can be a light filter, which filters out light of wavelengthshorter than 500 nm. Such effect can be achieved by coating on at leastone surface of the lens, or by using materials capable of filtering outshort waves to make the lens.

To meet different requirements, the image plane of the optical imagecapturing system in the present invention can be either flat or curved.If the image plane is curved (e.g., a sphere with a radius ofcurvature), the incidence angle required for focusing light on the imageplane can be decreased, which is not only helpful to shorten the lengthof the system (TTL), but also helpful to increase the relativeilluminance.

We provide several embodiments in conjunction with the accompanyingdrawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 ofthe first embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 110, an aperture100, a second lens 120, a third lens 130, a fourth lens 140, a fifthlens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter180, an image plane 190, and an image sensor 192. FIG. 1C shows amodulation transformation of the optical image capturing system 10 ofthe first embodiment of the present application in visible spectrum.

The first lens 110 has negative refractive power and is made of plastic.An object-side surface 112 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 114 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 112 has an inflection point, and the image-side surface 114 hastwo inflection points. A thickness of the first lens 110 on the opticalaxis is TP1, and a thickness of the first lens 110 at the height of ahalf of the entrance pupil diameter (HEP) is denoted by ETP1.

The first lens satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm; TP1=2.2761mm; |SGI111|/(|SGI111|+TP1)=0.0465; |SGI121|/(|SGI121|+TP1)=0.5437,where a displacement in parallel with the optical axis from a point onthe object-side surface of the first lens, through which the opticalaxis passes, to the inflection point on the image-side surface, which isthe closest to the optical axis is denoted by SGI111, and a displacementin parallel with the optical axis from a point on the image-side surfaceof the first lens, through which the optical axis passes, to theinflection point on the image-side surface, which is the closest to theoptical axis is denoted by SGI111.

The first lens satisfies SGI112=0 mm; SGI122=4.2315 mm;|SGI112|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where adisplacement in parallel with the optical axis from a point on theobject-side surface of the first lens, through which the optical axispasses, to the inflection point on the image-side surface, which is thesecond closest to the optical axis is denoted by SGI112, and adisplacement in parallel with the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to the inflection point on the image-side surface, which is thesecond closest to the optical axis is denoted by SGI122.

The first lens satisfies HIF111=12.8432 mm; HIF111/HOI=1.7127;HIF121=7.1744 mm; HIF121/HOI=0.9567, where a displacement perpendicularto the optical axis from a point on the object-side surface of the firstlens, through which the optical axis passes, to the inflection point,which is the closest to the optical axis is denoted by HIF111, and adisplacement perpendicular to the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to the inflection point, which is the closest to the opticalaxis is denoted by HIF121.

The first lens satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592 mm;HIF122/HOI=1.3147, where a displacement perpendicular to the opticalaxis from a point on the object-side surface of the first lens, throughwhich the optical axis passes, to the inflection point, which is thesecond closest to the optical axis is denoted by HIF112, and adisplacement perpendicular to the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to the inflection point, which is the second closest to theoptical axis is denoted by HIF122.

The second lens 120 has positive refractive power and is made ofplastic. An object-side surface 122 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 124thereof, which faces the image side, is a concave aspheric surface. Athickness of the second lens 120 on the optical axis is TP2, andthickness of the second lens 120 at the height of a half of the entrancepupil diameter (HEP) is denoted by ETP2.

For the second lens, a displacement in parallel with the optical axisfrom a point on the object-side surface of the second lens, throughwhich the optical axis passes, to the inflection point on the image-sidesurface, which is the closest to the optical axis is denoted by SGI211,and a displacement in parallel with the optical axis from a point on theimage-side surface of the second lens, through which the optical axispasses, to the inflection point on the image-side surface, which is theclosest to the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axisfrom a point on the object-side surface of the second lens, throughwhich the optical axis passes, to the inflection point, which is theclosest to the optical axis is denoted by HIF211, and a displacementperpendicular to the optical axis from a point on the image-side surfaceof the second lens, through which the optical axis passes, to theinflection point, which is the closest to the optical axis is denoted byHIF221.

The third lens 130 has negative refractive power and is made of plastic.An object-side surface 132, which faces the object side, is a convexaspheric surface, and an image-side surface 134, which faces the imageside, is a concave aspheric surface. A thickness of the third lens 130on the optical axis is TP3, and a thickness of the third lens 130 at theheight of a half of the entrance pupil diameter (HEP) is denoted byETP3.

For the third lens 130, SGI311 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the third lens,through which the optical axis passes, to the inflection point on theobject-side surface, which is the closest to the optical axis, andSGI321 is a displacement in parallel with the optical axis, from a pointon the image-side surface of the third lens, through which the opticalaxis passes, to the inflection point on the image-side surface, which isthe closest to the optical axis.

For the third lens 130, SGI312 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the third lens,through which the optical axis passes, to the inflection point on theobject-side surface, which is the second closest to the optical axis,and SGI322 is a displacement in parallel with the optical axis, from apoint on the image-side surface of the third lens, through which theoptical axis passes, to the inflection point on the object-side surface,which is the second closest to the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the closest to the optical axis, and theoptical axis; HIF321 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the second closest to the optical axis, and theoptical axis; HIF322 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the second closest to the optical axis, and the opticalaxis.

The fourth lens 140 has positive refractive power and is made ofplastic. An object-side surface 142, which faces the object side, is aconvex aspheric surface, and an image-side surface 144, which faces theimage side, is a convex aspheric surface. The object-side surface 142has an inflection point. A thickness of the fourth lens 140 on theoptical axis is TP4, and a thickness of the fourth lens 140 at theheight of a half of the entrance pupil diameter (HEP) is denoted byETP4.

The fourth lens 140 satisfies SGI411=0.0018 mm;|SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement inparallel with the optical axis, from a point on the object-side surfaceof the fourth lens, through which the optical axis passes, to theinflection point on the object-side surface, which is the closest to theoptical axis, and SGI421 is a displacement in parallel with the opticalaxis, from a point on the image-side surface of the fourth lens, throughwhich the optical axis passes, to the inflection point on the image-sidesurface, which is the closest to the optical axis.

For the fourth lens 140, SGI412 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the fourthlens, through which the optical axis passes, to the inflection point onthe object-side surface, which is the second closest to the opticalaxis, and SGI422 is a displacement in parallel with the optical axis,from a point on the image-side surface of the fourth lens, through whichthe optical axis passes, to the inflection point on the object-sidesurface, which is the second closest to the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm;HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the closest to the optical axis, and theoptical axis; HIF421 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the second closest to the optical axis, andthe optical axis; HIF422 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the second closest to the optical axis, and the opticalaxis.

The fifth lens 150 has positive refractive power and is made of plastic.An object-side surface 152, which faces the object side, is a concaveaspheric surface, and an image-side surface 154, which faces the imageside, is a convex aspheric surface. The object-side surface 152 and theimage-side surface 154 both have an inflection point. A thickness of thefifth lens 150 on the optical axis is TP5, and a thickness of the fifthlens 150 at the height of a half of the entrance pupil diameter (HEP) isdenoted by ETP5.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm;|SGI511|/(|SGI511|+TP5)=0.0284; |SGI521|/(|SGI521|+TP5)=0.3346, whereSGI511 is a displacement in parallel with the optical axis, from a pointon the object-side surface of the fifth lens, through which the opticalaxis passes, to the inflection point on the object-side surface, whichis the closest to the optical axis, and SGI521 is a displacement inparallel with the optical axis, from a point on the image-side surfaceof the fifth lens, through which the optical axis passes, to theinflection point on the image-side surface, which is the closest to theoptical axis.

For the fifth lens 150, SGI512 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the fifth lens,through which the optical axis passes, to the inflection point on theobject-side surface, which is the second closest to the optical axis,and SGI522 is a displacement in parallel with the optical axis, from apoint on the image-side surface of the fifth lens, through which theoptical axis passes, to the inflection point on the object-side surface,which is the second closest to the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm;HIF511/HOI=0.5091; HIF521/HOI=0.6065, where HIF511 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the fifth lens, which is the closest to theoptical axis, and the optical axis; HIF521 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the fifth lens, which is the closest to the optical axis, andthe optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fifth lens, which is the second closest to the optical axis, and theoptical axis; HIF522 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fifthlens, which is the second closest to the optical axis, and the opticalaxis.

The sixth lens 160 has negative refractive power and is made of plastic.An object-side surface 162, which faces the object side, is a convexaspheric surface, and an image-side surface 164, which faces the imageside, is a concave aspheric surface. The object-side surface 162 and theimage-side surface 164 both have an inflection point. Whereby, theincident angle of each view field entering the sixth lens 160 can beeffectively adjusted to improve aberration. A thickness of the sixthlens 160 on the optical axis is TP6, and a thickness of the sixth lens160 at the height of a half of the entrance pupil diameter (HEP) isdenoted by ETP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm;|SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, whereSGI611 is a displacement in parallel with the optical axis, from a pointon the object-side surface of the sixth lens, through which the opticalaxis passes, to the inflection point on the object-side surface, whichis the closest to the optical axis, and SGI621 is a displacement inparallel with the optical axis, from a point on the image-side surfaceof the sixth lens, through which the optical axis passes, to theinflection point on the image-side surface, which is the closest to theoptical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm;HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the sixth lens, which is the closest to theoptical axis, and the optical axis; HIF621 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the sixth lens, which is the closest to the optical axis, andthe optical axis.

The seventh lens 170 has positive refractive power and is made ofplastic. An object-side surface 172, which faces the object side, is aconvex aspheric surface, and an image-side surface 174, which faces theimage side, is a concave aspheric surface. The object-side surface 172and the image-side surface 174 both have an inflection point. Athickness of the seventh lens 170 on the optical axis is TP7, and athickness of the seventh lens 170 at the height of a half of theentrance pupil diameter (HEP) is denoted by ETP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm;|SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, whereSGI711 is a displacement in parallel with the optical axis, from a pointon the object-side surface of the seventh lens, through which theoptical axis passes, to the inflection point on the object-side surface,which is the closest to the optical axis, and SGI721 is a displacementin parallel with the optical axis, from a point on the image-sidesurface of the seventh lens, through which the optical axis passes, tothe inflection point on the image-side surface, which is the closest tothe optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the seventh lens, which is the closest to theoptical axis, and the optical axis; HIF721 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the seventh lens, which is the closest to the optical axis,and the optical axis.

A distance in parallel with the optical axis between a coordinate pointat a height of ½ HEP on the object-side surface of the first lens 110and the image plane is ETL, and a distance in parallel with the opticalaxis between the coordinate point at the height of ½ HEP on theobject-side surface of the first lens 110 and a coordinate point at aheight of ½ HEP on the image-side surface of the seventh lens 140 isEIN, which satisfies: ETL=26.980 mm; EIN=24.999 mm; EIN/ETL=0.927.

The optical image capturing system of the first embodiment satisfies:ETP1=2.470 mm; ETP2=5.144 mm; ETP3=0.898 mm; ETP4=1.706 mm; ETP5=3.901mm; ETP6=0.528 mm; ETP7=1.077 mm. The sum of the aforementioned ETP1 toETP7 is SETP, wherein SETP=15.723 mm. In addition, TP1=2.276 mm;TP2=5.240 mm; TP3=0.837 mm; TP4=2.002 mm; TP5=4.271 mm; TP6=0.300 mm;TP7=1.118 mm. The sum of the aforementioned TP1 to TP7 is STP, whereinSTP=16.044 mm. In addition, SETP/STP=0.980, and SETP/EIN=0.629.

In order to enhance the ability of correcting aberration and to lowerthe difficulty of manufacturing at the same time, the ratio between thethickness (ETP) at the height of a half of the entrance pupil diameter(HEP) and the thickness (TP) of any lens on the optical axis (i.e.,ETP/TP) in the optical image capturing system of the first embodiment isparticularly controlled, which satisfies: ETP1/TP1=1.085;ETP2/TP2=0.982; ETP3/TP3=1.073; ETP4/TP4=0.852; ETP5/TP5=0.914;ETP6/TP6=1.759; ETP7/TP7=0.963.

In order to enhance the ability of correcting aberration, lower thedifficulty of manufacturing, and “slightly shortening” the length of theoptical image capturing system at the same time, the ratio between thehorizontal distance (ED) between two neighboring lenses at the height ofa half of the entrance pupil diameter (HEP) and the parallel distance(IN) between these two neighboring lens on the optical axis (i.e.,ED/IN) in the optical image capturing system of the first embodiment isparticularly controlled, which satisfies: the horizontal distancebetween the first lens 110 and the second lens 120 at the height of ahalf of the entrance pupil diameter (HEP) is denoted by ED12, whereinED12=4.474 mm; the horizontal distance between the second lens 120 andthe third lens 130 at the height of a half of the entrance pupildiameter (HEP) is denoted by ED23, wherein ED23=0.349 mm; the horizontaldistance between the third lens 130 and the fourth lens 140 at theheight of a half of the entrance pupil diameter (HEP) is denoted byED34, wherein ED34=1.660 mm; the horizontal distance between the fourthlens 140 and the fifth lens 150 at the height of a half of the entrancepupil diameter (HEP) is denoted by ED45, wherein ED45=1.794 mm; thehorizontal distance between the fifth lens 150 and the sixth lens 160 atthe height of a half of the entrance pupil diameter (HEP) is denoted byED56, wherein ED56=0.714 mm; the horizontal distance between the sixthlens 160 and the seventh lens 170 at the height of a half of theentrance pupil diameter (HEP) is denoted by ED67, wherein ED67=0.284 mm.The sum of the aforementioned ED12 to ED67 is SED, wherein SED=9.276 mm.

The horizontal distance between the first lens 110 and the second lens120 on the optical axis is denoted by IN12, wherein IN12=4.552 mm, andED12/IN12=0.983. The horizontal distance between the second lens 120 andthe third lens 130 on the optical axis is denoted by IN23, whereinIN23=0.162 mm, and ED23/IN23=2.153. The horizontal distance between thethird lens 130 and the fourth lens 140 on the optical axis is denoted byIN34, wherein IN34=1.927 mm, and ED34/IN34=0.862. The horizontaldistance between the fourth lens 140 and the fifth lens 150 on theoptical axis is denoted by IN45, wherein IN45=1.515 mm, andED45/IN45=1.184. The horizontal distance between the fifth lens 150 andthe sixth lens 160 on the optical axis is denoted by IN56, whereinIN56=0.050 mm, and ED56/IN56=14.285. The horizontal distance between thesixth lens 160 and the seventh lens 170 on the optical axis is denotedby IN67, wherein IN67=0.211 mm, and ED67/IN67=1.345. The sum of theaforementioned IN12 to IN67 is denoted by SIN, wherein SIN=8.418, andSED/SIN=1.102.

The optical image capturing system of the first embodiment satisfies:ED12/ED23=12.816; ED23/ED34=0.210; ED34/ED45=0.925; ED45/ED56=2.512;ED56/ED67=2.512; IN12/IN23=28.080; IN23/IN34=0.084; IN34/IN45=1.272;IN45/IN56=30.305; IN56/IN67=0.236.

The horizontal distance in parallel with the optical axis between acoordinate point at the height of ½ HEP on the image-side surface of theseventh lens 170 and image surface is denoted by EBL, wherein EBL=1.982mm. The horizontal distance in parallel with the optical axis betweenthe point on the image-side surface of the seventh lens 170 where theoptical axis passes through and the image plane is denoted by BL,wherein BL=2.517 mm. The optical image capturing system of the firstembodiment satisfies: EBL/BL=0.7874. The horizontal distance in parallelwith the optical axis between the coordinate point at the height of ½HEP on the image-side surface of the seventh lens 170 and the infraredrays filter 180 is denoted by EIR, wherein EIR=0.865 mm. The horizontaldistance in parallel with the optical axis between the point on theimage-side surface of the seventh lens 170 where the optical axis passesthrough and the infrared rays filter 180 is denoted by PIR, whereinPIR=1.400 mm, and it satisfies: EIR/PIR=0.618.

The description below and the features related to inflection points areobtained based on main reference wavelength of 555 nm.

The infrared rays filter 180 is made of glass and between the seventhlens 170 and the image plane 190. The infrared rays filter 180 gives nocontribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has thefollowing parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968degrees; and tan(HAF)=1.7318, where f is a focal length of the system;HAF is a half of the maximum field angle; and HEP is an entrance pupildiameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm;|f/f1|=0.2961; f7=8.2933; |f1|>f7; and |f1/f7|=1.7519, where f1 is afocal length of the first lens 110; and f7 is a focal length of theseventh lens 170.

The first embodiment further satisfies|f2|+|f3|+|f4|+|f5|+|f6|=144.7494; |f1|+|f7|=22.8219 and|f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of thesecond lens 120, f3 is a focal length of the third lens 130, f4 is afocal length of the fourth lens 140, f5 is a focal length of the fifthlens 150, f6 is a focal length of the sixth lens 160, and f7 is a focallength of the seventh lens 170.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999;ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411;|f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=0.5187, where PPR is a ratio of afocal length f of the optical image capturing system to a focal lengthfp of each of the lenses with positive refractive power; and NPR is aratio of a focal length f of the optical image capturing system to afocal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment furthersatisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977;HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is adistance between the object-side surface 112 of the first lens 110 andthe image-side surface 174 of the seventh lens 170; HOS is a height ofthe image capturing system, i.e. a distance between the object-sidesurface 112 of the first lens 110 and the image plane 190; InS is adistance between the aperture 100 and the image plane 190; HOI is a halfof a diagonal of an effective sensing area of the image sensor 192,i.e., the maximum image height; and BFL is a distance between theimage-side surface 174 of the seventh lens 170 and the image plane 190.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of thethicknesses of the lenses 110-150 with refractive power. It is helpfulfor the contrast of image and yield rate of manufacture and provides asuitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment furthersatisfies |R1/R2|=129.9952, where R1 is a radius of curvature of theobject-side surface 112 of the first lens 110, and R2 is a radius ofcurvature of the image-side surface 114 of the first lens 110. Itprovides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment furthersatisfies (R13−R14)/(R13+R14)=−0.0806, where R13 is a radius ofcurvature of the object-side surface 172 of the seventh lens 170, andR14 is a radius of curvature of the image-side surface 174 of theseventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, whereΣPP is a sum of the focal lengths fp of each lens with positiverefractive power. It is helpful to share the positive refractive powerof the fourth lens 140 to other positive lenses to avoid the significantaberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNPis a sum of the focal lengths fn of each lens with negative refractivepower. It is helpful to share the negative refractive power of the firstlens 110 to the other negative lens, which avoid the significantaberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies IN12=4.5524 mm; IN12/f=1.0582, where IN12 is a distance on theoptical axis between the first lens 110 and the second lens 120. It maycorrect chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, whereTP1 is a central thickness of the first lens 110 on the optical axis,and TP2 is a central thickness of the second lens 120 on the opticalaxis. It may control the sensitivity of manufacture of the system andimprove the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, whereTP6 is a central thickness of the sixth lens 160 on the optical axis,TP7 is a central thickness of the seventh lens 170 on the optical axis,and IN67 is a distance on the optical axis between the sixth lens 160and the seventh lens 170. It may control the sensitivity of manufactureof the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment furthersatisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm;IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a centralthickness of the third lens 130 on the optical axis, TP4 is a centralthickness of the fourth lens 140 on the optical axis, TP5 is a centralthickness of the fifth lens 150 on the optical axis; IN34 is a distanceon the optical axis between the third lens 130 and the fourth lens 140;IN45 is a distance on the optical axis between the fourth lens 140 andthe fifth lens 150; InTL is a distance between the object-side surface112 of the first lens 110 and the image-side surface 174 of the seventhlens 170. It may control the sensitivity of manufacture of the systemand lower the total height of the system.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and |InRS62|/TP6=0.722,where InRS61 is a displacement in parallel with the optical axis from apoint on the object-side surface 162 of the sixth lens 160, throughwhich the optical axis passes, to a point at the maximum effective semidiameter of the object-side surface 162 of the sixth lens 160; InRS62 isa displacement in parallel with the optical axis from a point on theimage-side surface 164 of the sixth lens 160, through which the opticalaxis passes, to a point at the maximum effective semi diameter of theimage-side surface 164 of the sixth lens 160; and TP6 is a centralthickness of the sixth lens 160 on the optical axis. It is helpful formanufacturing and shaping of the lenses and is helpful to reduce thesize.

The optical image capturing system 10 of the first embodiment furthersatisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404,where HVT61 is a distance perpendicular to the optical axis between thecritical point on the object-side surface 162 of the sixth lens 160 andthe optical axis; and HVT62 is a distance perpendicular to the opticalaxis between the critical point on the image-side surface 164 of thesixth lens 160 and the optical axis.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm; and |InRS72|/TP7=0.0839,where InRS71 is a displacement in parallel with the optical axis from apoint on the object-side surface 172 of the seventh lens 170, throughwhich the optical axis passes, to a point at the maximum effective semidiameter of the object-side surface 172 of the seventh lens 170; InRS72is a displacement in parallel with the optical axis from a point on theimage-side surface 174 of the seventh lens 170, through which theoptical axis passes, to a point at the maximum effective semi diameterof the image-side surface 174 of the seventh lens 170; and TP7 is acentral thickness of the seventh lens 170 on the optical axis. It ishelpful for manufacturing and shaping of the lenses and is helpful toreduce the size.

The optical image capturing system 10 of the first embodiment satisfiesHVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 isa distance perpendicular to the optical axis between the critical pointon the object-side surface 172 of the seventh lens 170 and the opticalaxis; and HVT72 is a distance perpendicular to the optical axis betweenthe critical point on the image-side surface 174 of the seventh lens 170and the optical axis.

The optical image capturing system 10 of the first embodiment satisfiesHVT72/HOI=0.5414. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfiesHVT72/HOS=0.1505. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The second lens 120, the third lens 130, and the seventh lens 170 havenegative refractive power. The optical image capturing system 10 of thefirst embodiment further satisfies 1≦NA7/NA2, where NA2 is an Abbenumber of the second lens 120; NA3 is an Abbe number of the third lens130; and NA7 is an Abbe number of the seventh lens 170. It may correctthe aberration of the optical image capturing system.

The optical image capturing system 10 of the first embodiment furthersatisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; andODT is optical distortion.

For the optical image capturing system of the first embodiment, thevalues of MTF in the spatial frequency of 55 cycles/mm at the opticalaxis, 0.3 field of view, and 0.7 field of view of visible light on animage plane are respectively denoted by MTFE0, MTFE3, and MTFE7, whereinMTFE0 is around 0.35, MTFE3 is around 0.14, and MTEF7 is around 0.28;the values of MTF in the spatial frequency of 110 cycles/mm at theoptical axis, 0.3 field of view, and 0.7 field of view of visible lighton an image plane are respectively denoted by MTFQ0, MTFQ3, and MTFQ7,wherein MTFQ0 is around 0.126, MTFQ3 is around 0.075, and MTFQ7 isaround 0.177; the values of modulation transfer function (MTF) in thespatial frequency of 220 cycles/mm at the optical axis, 0.3 field ofview, and 0.7 field of view on an image plane are respectively denotedby MTFH0, MTFH3, and MTFH7, wherein MTFH0 is around 0.01, MTFH3 isaround 0.01, and MTFH7 is around 0.01.

For the optical image capturing system of the first embodiment, when theinfrared of wavelength of 850 nm focuses on the image plane, the valuesof MTF in spatial frequency (55 cycles/mm) at the optical axis, 0.3 HOI,and 0.7 HOI on an image plane are respectively denoted by MTFI0, MTFI3,and MTFI7, wherein MTFI0 is around 0.01, MTFI3 is around 0.01, and MTFI7is around 0.01.

The parameters of the lenses of the first embodiment are listed in Table1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2, HAF = 59.9968 deg Focal Radius ofThickness Refractive Abbe length Surface curvature (mm) (mm) Materialindex number (mm) 0 Object plane infinity 1 1^(st) lens −1079.4999642.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd)lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.009.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.867364751 0.300plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.917 18 Imageplane plane Reference wavelength (d-line): 555 mm.

TABLE2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k2.500000E+01 −4.711931E−01 1.531617E+00 −1.153034E+01 −2.915013E+004.886991E+00 −3.459463E+01 A4 5.236918E−06 −2.117558E−04 7.146736E−054.353586E−04 5.793768E−04 −3.756697E−04 −1.292614E−03 A6 −3.014384E−08−1.838670E−06 2.334364E−06 1.400287E−05 2.112652E−04 3.901218E−04−1.602381E−05 A8 −2.487400E−10 9.605910E−09 −7.479362E−08 −1.688929E−07−1.344586E−05 −4.925422E−05 −8.452359E−06 A10 1.170000E−12 −8.256000E−111.701570E−09 3.829807E−08 1.000482E−06 4.139741E−06 7.243999E−07 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 1213 14 15 k −7.549291E+00 −5.000000E+01 −1.740728E+00 −4.709650E+00−4.509781E+00 −3.427137E+00 −3.215123E+00 A4 −5.583548E−03 1.240671E−046.467538E−04 −1.872317E−03 −8.967310E−04 −3.189453E−03 −2.815022E−03 A61.947110E−04 −4.949077E−05 −4.981838E−05 −1.523141E−05 −2.688331E−05−1.058126E−05 1.884580E−05 A8 −1.486947E−05 2.088854E−06 9.129031E−07−2.169414E−06 −8.324958E−07 1.760103E−06 −1.017223E−08 A10 −6.501246E−08−1.438383E−08 7.108550E−09 −2.308304E−08 −6.184250E−09 −4.730294E−083.660000E−12 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

The detail parameters of the first embodiment are listed in Table 1, inwhich the unit of the radius of curvature, thickness, and focal lengthare millimeter, and surface 0-10 indicates the surfaces of all elementsin the system in sequence from the object side to the image side. Table2 is the list of coefficients of the aspheric surfaces, in which A1-A20indicate the coefficients of aspheric surfaces from the first order tothe twentieth order of each aspheric surface. The following embodimentshave the similar diagrams and tables, which are the same as those of thefirst embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 ofthe second embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 210, asecond lens 220, a third lens 230, an aperture 200, a fourth lens 240, afifth lens 250, a sixth lens 260, a seventh lens 270, an infrared raysfilter 280, an image plane 290, and an image sensor 292. FIG. 2C shows amodulation transformation of the optical image capturing system 20 ofthe second embodiment of the present application in visible spectrum.

The first lens 210 has negative refractive power and is made of glass.An object-side surface 212 thereof, which faces the object side, is aconvex surface, and an image-side surface 214 thereof, which faces theimage side, is a concave surface.

The second lens 220 has negative refractive power and is made of glass.An object-side surface 222 thereof, which faces the object side, is aconcave surface, and an image-side surface 224 thereof, which faces theimage side, is a concave surface.

The third lens 230 has positive refractive power and is made of glass.An object-side surface 232, which faces the object side, is a convexsurface, and an image-side surface 234, which faces the image side, is aconvex surface.

The fourth lens 240 has positive refractive power and is made ofplastic. An object-side surface 242, which faces the object side, is aconvex surface, and an image-side surface 244, which faces the imageside, is a convex surface.

The fifth lens 250 has negative refractive power and is made of glass.An object-side surface 252, which faces the object side, is a concavesurface, and an image-side surface 254, which faces the image side, is aconcave surface.

The sixth lens 260 has positive refractive power and is made of glass.An object-side surface 262, which faces the object side, is a convexsurface, and an image-side surface 254, which faces the image side, is aconvex surface. Whereby, the incident angle of each view field enteringthe sixth lens 260 can be effectively adjusted to improve aberration.

The seventh lens 270 has positive refractive power and is made ofplastic. An object-side surface 272, which faces the object side, is aconvex surface, and an image-side surface 274, which faces the imageside, is a concave surface. It may help to shorten the back focal lengthto keep small in size. In addition, it may reduce an incident angle ofthe light of an off-axis field of view and correct the aberration of theoff-axis field of view.

The infrared rays filter 280 is made of glass and between the seventhlens 270 and the image plane 290. The infrared rays filter 280 gives nocontribution to the focal length of the system.

The parameters of the lenses of the second embodiment are listed inTable 3 and Table 4.

TABLE 3 f = 3.5645 mm; f/HEP = 1.2; HAF = 100 deg Focal Radius ofThickness Refractive Abbe length Surface curvature (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 81.26661295 7.298glass 1.723 37.96 −21.885 2 12.80057917 8.737 3 2^(nd) lens −47.015470622.713 glass 1.540 59.46 −16.148877 4 10.96331907 4.870 5 3^(rd) lens−49.73416268 13.867 glass 2.003 19.32 38.256 6 −24.82210772 14.233 7Aperture 1E+18 −1.398 8 4^(th) lens 12.66765795 3.491 plastic 1.56558.00 13.658275 9 −17.92107944 3.210 10 5^(th) lens −37.35459919 0.786glass 2.003 19.32 −10.800 11 15.61403391 3.269 12 6^(th) lens28.43288407 6.271 glass 1.497 81.61 19.20995 13 −13.36462224 0.050 147^(th) lens 9.405612213 10.000 plastic 1.565 58.00 19.728466 1536.44028077 1.300 16 Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 171E+18 0.999 18 Image 1E+18 0.005 plane Reference wavelength (d-line):555 nm

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 −2.087497E+00 A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 6.743050E−05 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−1.015201E−07 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 −2.069615E−09 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 3.483293E−12 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k −9.006424E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −3.596676E−01 −2.501625E+01 A4−8.398295E−05 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+002.582157E−05 6.675425E−04 A6 1.769062E−06 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 8.225359E−07 −4.723930E−06 A8 −2.620873E−080.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −7.975991E−094.032167E−07 A10 1.829963E−10 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 1.339976E−10 −2.321706E−09 A12 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the second embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the second embodiment based on Table 3 and Table4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4ETP5 ETP6 7.371 2.837 13.845 3.343 0.886 6.150 ETP7 ETL EBL EIN EIR PIR9.915 79.986 2.570 77.416 1.267 1.300 EIN/ETL SETP/EIN EIR/PIR SETP STPSETP/STP 0.968 0.573 0.974 44.347 44.426 0.998 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.010 1.046 0.998 0.958 1.128 0.981ETP7/TP7 BL EBL/BL SED SIN SED/SIN 0.992 2.603 0.987 33.069 32.971 1.003ED12 ED23 ED34 ED45 ED56 ED67 8.627 4.747 12.966 3.242 3.237 0.251 ED12/ED34/ ED56/ IN12 ED23/IN23 IN34 ED45/IN45 IN56 ED67/IN67 0.987 0.9751.010 1.010 0.990 5.013 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.16290.2207 0.0932 0.2610 0.3300 0.1856 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/fIN67/f 0.1807 0.7204 0.7136 1.0095 2.4511 0.0140 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP7 + IN67)/TP6 1.3552 0.4221 5.9111 1.6025 HOS InTL HOS/HOIInS/HOS ODT % TDT % 79.9999 77.3966 16.0000 0.3535 −124.7720 96.7361HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.00000.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.00000.0000 0.0000 0.0000 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9 0.8 0.80.73 0.44 0.47

The results of the equations of the second embodiment based on Table 3and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment(Reference wavelength: 555 nm) HIF221 0 HIF221/HOI 0 SGI221 0 |SGI221|/0 (|SGI221| + TP2)

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system ofthe third embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 310, a secondlens 320, a third lens 330, an aperture 300, a fourth lens 340, a fifthlens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter380, an image plane 390, and an image sensor 392. FIG. 3C shows amodulation transformation of the optical image capturing system 30 ofthe third embodiment of the present application in visible spectrum.

The first lens 310 has negative refractive power and is made of glass.An object-side surface 312 thereof, which faces the object side, is aconvex surface, and an image-side surface 314 thereof, which faces theimage side, is a concave surface.

The second lens 320 has negative refractive power and is made of glass.An object-side surface 322 thereof, which faces the object side, is aconcave surface, and an image-side surface 324 thereof, which faces theimage side, is a concave surface.

The third lens 330 has positive refractive power and is made of glass.An object-side surface 332 thereof, which faces the object side, is aconvex surface, and an image-side surface 334 thereof, which faces theimage side, is a convex surface.

The fourth lens 340 has positive refractive power and is made ofplastic. An object-side surface 342, which faces the object side, is aconvex aspheric surface, and an image-side surface 344, which faces theimage side, is a convex aspheric surface. The object-side surface 345has an inflection point.

The fifth lens 350 has negative refractive power and is made of glass.An object-side surface 352, which faces the object side, is a concavesurface, and an image-side surface 354, which faces the image side, is aconcave surface

The sixth lens 360 has positive refractive power and is made of glass.An object-side surface 362, which faces the object side, is a convexsurface, and an image-side surface 364, which faces the image side, is aconvex surface. Whereby, the incident angle of each view field enteringthe sixth lens 360 can be effectively adjusted to improve aberration.

The seventh lens 370 has positive refractive power and is made ofplastic. An object-side surface 372, which faces the object side, is aconvex surface, and an image-side surface 374, which faces the imageside, is a concave surface. It may help to shorten the back focal lengthto keep small in size. In addition, it may reduce an incident angle ofthe light of an off-axis field of view and correct the aberration of theoff-axis field of view.

The infrared rays filter 380 is made of glass and between the seventhlens 370 and the image plane 390. The infrared rays filter 390 gives nocontribution to the focal length of the system.

The parameters of the lenses of the third embodiment are listed in Table5 and Table 6.

TABLE 5 f = 4.4869 mm; f/HEP = 1.2; HAF = 70.0012 deg Radius ofThickness Refractive Abbe Focal length Surface curvature (mm) (mm)Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens26.04397949 1.749 glass 1.618 49.82 −23.588 2 9.12476488 6.648 3 2^(nd)lens −24.36336093 1.974 glass 1.517 64.20 −12.314429 4 8.886733083 3.4745 3^(rd) lens 53.4804248 15.990 glass 2.001 29.13 13.774 6 −15.92176181−0.906 7 Aperture 1E+18 2.186 8 4^(th) lens 42.93756248 6.318 plastic1.565 58.00 15.616502 9 −10.55595881 0.050 10 5^(th) lens −15.849886161.082 glass 2.003 19.32 −10.479 11 33.14881544 2.052 12 6^(th) lens35.16946959 7.296 glass 1.497 81.61 19.705845 13 −12.67666575 0.050 147^(th) lens 9.087321757 9.435 plastic 1.565 58.00 26.217666 1514.60745978 1.000 16 Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 171E+18 1.309 18 Image 1E+18 −0.006 plane Reference wavelength (d-line):555 nm.

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 −4.810363E+01 A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −1.541186E−04 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−5.488822E−06 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 1.022833E−07 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −3.988831E−09 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k 3.474113E−01 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −2.246088E+00 −1.615053E+01 A4−1.529356E−04 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+002.592427E−04 7.490079E−04 A6 3.184182E−06 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 −5.186554E−07 −2.241914E−05 A8 −4.357874E−080.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 7.376083E−098.604405E−07 A10 −1.020702E−10 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 3.518355E−11 −8.058894E−09 A12 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the third embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the third embodiment based on Table 5 and Table6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4 ETP5ETP6 1.875 2.245 15.847 6.112 1.246 7.108 ETP7 ETL EBL EIN EIR PIR 9.36359.933 2.482 57.451 0.879 1.000 EIN/ETL SETP/EIN EIR/PIR SETP STPSETP/STP 0.959 0.762 0.879 43.795 43.844 0.999 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.072 1.137 0.991 0.967 1.151 0.974ETP7/TP7 BL EBL/BL SED SIN SED/SIN 0.992 2.603 0.954 13.656 13.553 1.008ED12 ED23 ED34 ED45 ED56 ED67 6.382 3.308 1.428 0.108 2.048 0.382 ED12/ED34/ ED56/ IN12 ED23/IN23 IN34 ED45/IN45 IN56 ED67/IN67 0.960 0.9521.116 2.169 0.999 7.632 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.19020.3644 0.3258 0.2873 0.4282 0.2277 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/fIN67/f 0.1711 1.0119 0.9827 1.0297 1.4816 0.0111 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP7 + IN67)/TP6 1.9155 0.8940 4.2529 1.3000 HOS InTL HOS/HOIInS/HOS ODT % TDT % 59.9999 57.3968 12.0000 0.5179 −59.4432 41.5180HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.00000.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.00000.0000 0.0000 0.0000 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9 0.8 0.80.74 0.44 0.47

The results of the equations of the third embodiment based on Table 5and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment(Reference wavelength: 555 nm) HIF411 2.5699 HIF411/HOI 0.5140 SGI4110.0658 |SGI411|/(|SGI411| + TP4) 0.0103

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 ofthe fourth embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 410, asecond lens 420, a third lens 430, an aperture 400, a fourth lens 440, afifth lens 450, a sixth lens 460, a seventh lens 470, an infrared raysfilter 480, an image plane 490, and an image sensor 492. FIG. 4C shows amodulation transformation of the optical image capturing system 40 ofthe fourth embodiment of the present application in visible spectrum.

The first lens 410 has negative refractive power and is made of glass.An object-side surface 412 thereof, which faces the object side, is aconvex surface, and an image-side surface 414 thereof, which faces theimage side, is a concave surface.

The second lens 420 has negative refractive power and is made of glass.An object-side surface 422 thereof, which faces the object side, is aconcave surface, and an image-side surface 424 thereof, which faces theimage side, is a concave surface.

The third lens 430 has positive refractive power and is made of glass.An object-side surface 432 thereof, which faces the object side, is aconvex surface, and an image-side surface 434 thereof, which faces theimage side, is a convex surface.

The fourth lens 440 has positive refractive power and is made of glass.An object-side surface 442, which faces the object side, is a convexsurface, and an image-side surface 444, which faces the image side, is aconvex surface.

The fifth lens 450 has negative refractive power and is made of glass.An object-side surface 452, which faces the object side, is a concavesurface, and an image-side surface 454, which faces the image side, is aconcave surface.

The sixth lens 460 has positive refractive power and is made of plastic.An object-side surface 462, which faces the object side, is a convexsurface, and an image-side surface 464, which faces the image side, is aconvex surface. The image-side surface 464 has an inflection point.Whereby, the incident angle of each view field entering the sixth lens460 can be effectively adjusted to improve aberration.

The seventh lens 470 has positive refractive power and is made ofplastic. An object-side surface 472, which faces the object side, is aconvex surface, and an image-side surface 474, which faces the imageside, is a concave surface. It may help to shorten the back focal lengthto keep small in size. In addition, the image-side surface 474 has aninflection point, which may reduce an incident angle of the light of anoff-axis field of view and correct the aberration of the off-axis fieldof view.

The infrared rays filter 480 is made of glass and between the seventhlens 470 and the image plane 490. The infrared rays filter 480 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fourth embodiment are listed inTable 7 and Table 8.

TABLE 7 f = 3.8739 mm; f/HEP = 1.4; HAF = 89.9490 deg Focal Radius ofThickness Refractive Abbe length Surface curvature (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 55.06878721 6.570glass 1.702 41.15 −11.628 2 6.78062347 5.185 3 2^(nd) lens −14.67806161.427 glass 1.571 52.95 −9.762421 4 9.36714717 1.068 5 3^(rd) lens24.43967035 14.119 glass 1.904 31.32 13.228 6 −17.15498053 −0.537 7Aperture 1E+18 1.158 8 4^(th) lens 9.023094755 3.624 glass 1.564 60.6712.357953 9 −26.50322763 2.102 10 5^(th) lens −15.56787679 0.773 glass0.946 17.98 −8.659 11 18.08001764 0.191 12 6^(th) lens 11.30892753 3.141plastic 1.565 58.00 19.671677 13 −711.4772483 1.661 14 7^(th) lens5.996117623 7.999 plastic 1.565 58.00 11.419453 15 42.16794691 1.000 16Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 17 1E+18 0.133 18 Image1E+18 0.003 plane Reference wavelength (d-line): 555 nm.

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 0.000000E+000.000000E+00 −9.126673E+00 5.000000E+01 −3.202270E+00 5.000000E+01 A40.000000E+00 0.000000E+00 0.000000E+00 7.375850E−04 −8.882921E−042.855718E−04 7.822408E−05 A6 0.000000E+00 0.000000E+00 0.000000E+00−8.049705E−06 6.500490E−05 4.287775E−06 −2.358328E−05 A8 0.000000E+000.000000E+00 0.000000E+00 2.221418E−07 −1.586885E−06 −2.085766E−077.754415E−08 A10 0.000000E+00 0.000000E+00 0.000000E+00 1.283089E−092.909062E−08 2.245479E−09 4.673762E−09 A12 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the fourth embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the fourth embodiment based on Table 7 and Table8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4ETP5 ETP6 6.695 1.596 14.024 3.481 0.888 3.052 ETP7 ETL EBL EIN EIR PIR7.866 49.899 1.412 48.487 0.977 1.000 EIN/ETL SETP/EIN EIR/PIR SETP STPSETP/STP 0.972 0.775 0.977 37.601 37.653 0.999 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.019 1.118 0.993 0.961 1.148 0.972ETP7/TP7 BL EBL/BL SED SIN SED/SIN 0.983 1.435 0.984 10.886 10.828 1.005ED12 ED23 ED34 ED45 ED56 ED67 4.977 1.004 0.784 2.076 0.223 1.821 ED12/ED34/ ED56/ IN12 ED23/IN23 IN34 ED45/IN45 IN56 ED67/IN67 0.960 0.9401.262 0.988 1.166 1.097 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.33310.3968 0.2928 0.3135 0.4474 0.1969 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/fIN67/f 0.3392 1.1425 1.1773 0.9704 1.3385 0.4287 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP7 + IN67)/TP6 1.1911 0.7380 8.2348 3.0753 HOS InTL HOS/HOIInS/HOS ODT % TDT % 49.9163 48.4811 9.9833 0.4424 −100.1150 74.2108HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.00000.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 3.6678 0.00004.3798 0.8760 0.0877 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9 0.88 0.820.74 0.68 0.54

The results of the equations of the fourth embodiment based on Table 7and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment(Reference wavelength: 555 nm) HIF621 2.7580 HIF621/HOI 0.5516 SGI621−0.0327 |SGI621|/(|SGI621| + TP6) 0.0103 HIF721 2.8603 HIF721/HOI 0.5721SGI721 0.0963 |SGI721|/(|SGI721| + TP7) 0.0119

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system ofthe fifth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 510, a secondlens 520, a third lens 530, an aperture 500, a fourth lens 540, a fifthlens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter580, an image plane 590, and an image sensor 592. FIG. 5C shows amodulation transformation of the optical image capturing system 50 ofthe fifth embodiment of the present application in visible spectrum, andFIG. 5D shows a modulation transformation of the optical image capturingsystem 50 of the fifth embodiment of the present application in infraredspectrum.

The first lens 510 has negative refractive power and is made of glass.An object-side surface 512, which faces the object side, is a convexsurface, and an image-side surface 514, which faces the image side, is aconcave surface.

The second lens 520 has negative refractive power and is made ofplastic. An object-side surface 522 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 524thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 522 has an inflection point.

The third lens 530 has positive refractive power and is made of glass.An object-side surface 532, which faces the object side, is a concavesurface, and an image-side surface 534, which faces the image side, is aconvex surface.

The fourth lens 540 has positive refractive power and is made of glass.An object-side surface 542, which faces the object side, is a convexsurface, and an image-side surface 544, which faces the image side, is aconvex surface.

The fifth lens 550 has negative refractive power and is made of glass.An object-side surface 552, which faces the object side, is a concavesurface, and an image-side surface 554, which faces the image side, is aconcave surface.

The sixth lens 560 has positive refractive power and is made of glass.An object-side surface 562, which faces the object side, is a convexsurface, and an image-side surface 564, which faces the image side, is aconvex surface. Whereby, the incident angle of each view field enteringthe sixth lens 560 can be effectively adjusted to improve aberration.

The seventh lens 570 has positive refractive power and is made ofplastic. An object-side surface 572, which faces the object side, is aconvex aspheric surface, and an image-side surface 574, which faces theimage side, is a concave aspheric surface. The object-side surface 572has an inflection point. It may help to shorten the back focal length tokeep small in size.

The infrared rays filter 580 is made of glass and between the seventhlens 570 and the image plane 590. The infrared rays filter 580 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fifth embodiment are listed in Table9 and Table 10.

TABLE 9 f = 3.2083 mm; f/HEP = 1.4; HAF = 89.9474 deg Focal Radius ofThickness Refractive Abbe length Surface curvature (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 83.96518516 7.241glass 1.618 49.82 −17.575 2 9.326358432 3.534 3 2^(nd) lens 11.022142111.521 plastic 1.565 58.00 −12.872126 4 4.170734261 5.091 5 3^(rd) lens−150.4983169 15.587 glass 1.904 31.32 19.261 6 −16.45491092 3.848 7Aperture 1E+18 −0.931 8 4^(th) lens 8.004786547 1.960 glass 1.497 81.6112.313954 9 −24.10487564 1.315 10 5^(th) lens −16.57233815 0.302 glass2.003 19.32 −12.467 11 53.33317594 0.050 12 6^(th) lens 8.0474294692.213 glass 1.497 81.61 13.735755 13 −41.49798653 2.951 14 7^(th) lens7.762139792 1.894 plastic 1.565 58.00 42.820864 15 10.40443208 1.000 16Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 17 1E+18 2.120 18 Image1E+18 0.003 plane Reference wavelength (d-line): 555 nm.

TABLE 10 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 −4.060850E+00 −7.471441E−01 0.000000E+000.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 4.751371E−048.049739E−04 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+000.000000E+00 −2.025884E−05 −9.449005E−06 0.000000E+00 0.000000E+000.000000E+00 A8 0.000000E+00 0.000000E+00 2.307831E−07 −8.340413E−070.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00−8.732409E−10 1.642162E−08 0.000000E+00 0.000000E+00 0.000000E+00 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −5.586348E+00 8.151493E−01 A40.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−3.840736E−04 −6.745706E−05 A6 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 −5.228580E−05 −6.182507E+05 A8 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −9.780278E−06−5.640611E−06 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 3.755641E−07 3.911371E−07 A12 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the fifth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the fifth embodiment based on Table 9 and Table10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4 ETP5ETP6 7.304 1.621 15.551 1.850 0.354 2.115 ETP7 ETL EBL EIN EIR PIR 1.87649.992 3.360 46.632 0.937 1.000 EIN/ETL SETP/EIN EIR/PIR SETP STPSETP/STP 0.933 0.658 0.937 30.672 30.719 0.998 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.009 1.066 0.998 0.944 1.172 0.956ETP7/TP7 BL EBL/BL SED SIN SED/SIN 0.990 3.423 0.982 15.960 15.857 1.006ED12 ED23 ED34 ED45 ED56 ED67 3.523 4.927 3.039 1.303 0.120 3.049 ED12/ED34/ ED56/ IN12 ED23/IN23 IN34 ED45/IN45 IN56 ED67/IN67 0.997 0.9681.042 0.991 2.394 1.033 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.18250.2492 0.1666 0.2605 0.2573 0.2336 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/fIN67/f 0.0749 0.7356 0.6891 1.0674 1.1015 0.9198 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP7 + IN67)/TP6 1.3654 0.6683 7.0825 2.1895 HOS InTL HOS/HOIInS/HOS ODT % TDT % 49.9998 46.5765 10.0000 0.2636 −100.1430 72.9560HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.00000.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 3.24370.0000 0.0000 0.0000 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.88 0.88 0.820.7 0.69 0.52

The results of the equations of the fifth embodiment based on Table 9and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment(Reference wavelength: 555 nm) HIF211 4.6478 HIF211/HOI 0.9296 SGI2110.9375 |SGI211|/(|SGI211| + TP2) 0.3813 HIF711 2.0919 HIF711/HOI 0.4184SGI711 0.246933 |SGI711|/(|SGI711| + TP7) 0.1153 HIF721 2.6071HIF721/HOI 0.5214 SGI721 0.307611 |SGI721|/(|SGI721| + TP7) 0.1397HIF722 3.3476 HIF722/HOI 0.6695 SGI722 0.4512 |SGI722|/(|SGI722| + TP7)0.1924

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system ofthe sixth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 610, a secondlens 620, a third lens 630, an aperture 600, a fourth lens 640, a fifthlens 650, a sixth lens 660, a seventh lens 670, an infrared rays filter680, an image plane 690, and an image sensor 692. FIG. 6C shows amodulation transformation of the optical image capturing system 60 ofthe sixth embodiment of the present application in visible spectrum.

The first lens 610 has negative refractive power and is made of glass.An object-side surface 612, which faces the object side, is a convexsurface, and an image-side surface 614, which faces the image side, is aconcave surface.

The second lens 620 has negative refractive power and is made of glass.An object-side surface 622 thereof, which faces the object side, is aconcave surface, and an image-side surface 624 thereof, which faces theimage side, is a concave surface.

The third lens 630 has positive refractive power and is made of plastic.An object-side surface 632, which faces the object side, is a convexaspheric surface, and an image-side surface 634, which faces the imageside, is a convex aspheric surface.

The fourth lens 640 has positive refractive power and is made of glass.An object-side surface 642, which faces the object side, is a convexsurface, and an image-side surface 644, which faces the image side, is aconvex surface.

The fifth lens 650 has negative refractive power and is made of plastic.An object-side surface 652, which faces the object side, is a concaveaspheric surface, and an image-side surface 654, which faces the imageside, is a concave aspheric surface.

The sixth lens 660 has positive refractive power and is made of glass.An object-side surface 662, which faces the object side, is a convexsurface, and an image-side surface 664, which faces the image side, is aconvex surface. Whereby, the incident angle of each view field enteringthe sixth lens 660 can be effectively adjusted to improve aberration.

The seventh lens 670 has positive refractive power and is made of glass.An object-side surface 672, which faces the object side, is a convexsurface, and an image-side surface 674, which faces the image side, is aconcave surface. It may help to shorten the back focal length to keepsmall in size. In addition, it may reduce an incident angle of the lightof an off-axis field of view and correct the aberration of the off-axisfield of view.

The infrared rays filter 680 is made of glass and between the seventhlens 670 and the image plane 690. The infrared rays filter 680 gives nocontribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table11 and Table 12.

TABLE 11 f = 3.7144 mm; f/HEP = 1.4; HAF = 89.9470 deg Focal Radius ofThickness Refractive Abbe length Surface curvature (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 55.395572 2.502glass 1.517 64.20 −23.690518 2 9.895564402 6.448 3 2^(nd) lens−50.53624354 2.081 glass 1.517 64.20 −11.08541 4 6.573286609 8.420 53^(rd) lens 24.92472538 12.864 plastic 1.565 58.00 13.192558 6−8.687444677 −1.233 7 Aperture 1E+18 1.283 8 4^(th) lens 9.6461590756.395 glass 1.517 64.20 11.522512 9 −12.12977359 0.050 10 5^(th) lens−42.02401278 1.473 plastic 1.650 21.40 −6.868451 11 5.111986966 1.465 126^(th) lens 11.31865697 1.738 glass 1.497 81.61 21.229661 13−152.6762488 1.740 14 7^(th) lens 8.904426344 2.955 glass 1.497 81.6120.192241 15 69.07278594 1.000 16 Infrared 1E+18 0.300 BK_7 1.517 64.2rays filter 17 1E+18 0.385 18 Image 1E+18 −0.001 plane Referencewavelength (d-line): 555 nm.

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −2.789256E+01−4.698811E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 1.499980E−04 −5.092334E−04 0.000000E+00 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −2.861642E−06 1.354344E−050.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+005.906651E−08 −2.914722E−07 0.000000E+00 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 3.471310E−10 3.827772E−09 0.000000E+00 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 5.000000E+01−2.719616E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A40.000000E+00 −5.624739E−04 9.508751E−04 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A6 0.000000E+00 5.108089E−06 −3.254204E−050.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 0.000000E+007.292896E−09 1.433719E−06 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A10 0.000000E+00 −5.448557E−10 −2.493233E−08 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the sixth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the sixth embodiment based on Table 11 and Table12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4 ETP5ETP6 2.575 2.233 12.728 6.230 1.666 1.655 ETP7 ETL EBL EIN EIR PIR 2.86849.847 1.671 48.176 0.987 1.000 EIN/ETL SETP/EIN EIR/PIR SETP STPSETP/STP 0.966 0.622 0.987 29.955 30.007 0.998 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.029 1.073 0.989 0.974 1.131 0.952ETP7/TP7 BL EBL/BL SED SIN SED/SIN 0.971 1.684 0.992 18.220 18.172 1.003ED12 ED23 ED34 ED45 ED56 ED67 6.341 8.320 0.242 0.100 1.373 1.845 ED45/ED56/ ED67/ ED12/IN12 ED23/IN23 ED34/IN34 IN45 IN56 IN67 0.983 0.9884.847 1.997 0.937 1.060 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.15680.3351 0.2816 0.3224 0.5408 0.1750 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/fIN67/f 0.1840 0.9628 1.0327 0.9324 1.7358 0.4684 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP7 + IN67)/TP6 2.1371 0.8403 4.3013 2.7006 HOS InTL HOS/HOIInS/HOS ODT % TDT % 49.8628 48.1789 9.9726 0.3767 −100.1240 73.2060HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.00000.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.00000.0000 0.0000 0.0000 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.92 0.88 0.850.8 0.72 0.62

The results of the equations of the sixth embodiment based on Table 11and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment(Reference wavelength: 555 nm) HIF311 0 HIF311/HOI 0 SGI311 0 |SGI311|/0 (|SGI311| + TP3)

Seventh Embodiment

As shown in FIG. 7A and FIG. 7B, an optical image capturing system ofthe seventh embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 710, asecond lens 720, a third lens 730, an aperture 700, a fourth lens 740, afifth lens 750, a sixth lens 760, a seventh lens 770, an infrared raysfilter 780, an image plane 790, and an image sensor 792. FIG. 7C shows amodulation transformation of the optical image capturing system 70 ofthe seventh embodiment of the present application in visible spectrum.

The first lens 710 has negative refractive power and is made of glass.An object-side surface 712, which faces the object side, is a convexsurface, and an image-side surface 714, which faces the image side, is aconcave surface.

The second lens 720 has negative refractive power and is made of glass.An object-side surface 722 thereof, which faces the object side, is aconcave surface, and an image-side surface 724 thereof, which faces theimage side, is a concave surface.

The third lens 730 has positive refractive power and is made of plastic.An object-side surface 732, which faces the object side, is a convexaspheric surface, and an image-side surface 734, which faces the imageside, is a convex aspheric surface.

The fourth lens 740 has positive refractive power and is made ofplastic. An object-side surface 742, which faces the object side, is aconvex aspheric surface, and an image-side surface 744, which faces theimage side, is a convex aspheric surface.

The fifth lens 750 has negative refractive power and is made of glass.An object-side surface 752, which faces the object side, is a concavesurface, and an image-side surface 754, which faces the image side, is aconcave surface.

The sixth lens 760 has positive refractive power and is made of glass.An object-side surface 762, which faces the object side, is a convexsurface, and an image-side surface 764, which faces the image side, is aconcave surface. Whereby, the incident angle of each view field enteringthe sixth lens 760 can be effectively adjusted to improve aberration.

The seventh lens 770 has positive refractive power and is made of glass.An object-side surface 772, which faces the object side, is a convexsurface, and an image-side surface 774, which faces the image side, is aconcave surface. It may help to shorten the back focal length to keepsmall in size. In addition, it may reduce an incident angle of the lightof an off-axis field of view and correct the aberration of the off-axisfield of view.

The infrared rays filter 780 is made of glass and between the seventhlens 770 and the image plane 790. The infrared rays filter 780 gives nocontribution to the focal length of the system.

The parameters of the lenses of the seventh embodiment are listed inTable 13 and Table 14.

TABLE 13 f = 3.5483 mm; f/HEP = 1.4; HAF = 89.9439 deg Focal Radius ofThickness Refractive Abbe length Surface curvature (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 66.17875198 2.175glass 1.569 56.04 −20.004873 2 9.620453189 6.061 3 2^(nd) lens−68.64268359 2.043 glass 1.497 81.61 −12.349259 4 6.823660148 10.858 53^(rd) lens 16.41979029 10.144 plastic 1.565 58.00 13.157055 6−10.60847856 −0.602 7 Aperture 1E+18 2.497 8 4^(th) lens 7.7632209854.232 plastic 1.565 58.00 8.776302 9 −11.11542134 0.050 10 5^(th) lens−60.62447362 3.077 glass 2.003 19.32 −5.51332 11 6.301812305 1.718 126^(th) lens 9.331032499 1.424 glass 1.497 81.61 25.975169 13 31.768655631.049 14 7^(th) lens 11.13231175 0.968 glass 2.001 29.13 22.219909 1521.18447334 1.000 16 Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 171E+18 0.632 18 Image 1E+18 −0.002 plane Reference wavelength (d-line):555 nm.

TABLE 14 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −1.358636E+01−5.641282E+00 −8.337465E−01 A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 2.426764E−04 −5.957400E−04 −1.959381E−04 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −6.480474E−06 1.969887E−057.487283E−06 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+001.126110E−07 −4.379910E−07 −2.410507E−07 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 2.676202E−11 6.107990E−09 2.565746E−09 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k 1.738905E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A43.500925E−04 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A6 8.355636E−06 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 −2.389796E−070.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A10 5.462664E−09 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the seventh embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the seventh embodiment based on Table 13 andTable 14 are listed in the following table:

Seventh embodiment (Reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4ETP5 ETP6 2.247 2.173 10.020 4.057 3.219 1.363 ETP7 ETL EBL EIN EIR PIR0.933 47.611 1.892 45.719 0.962 1.000 EIN/ETL SETP/EIN EIR/PIR SETP STPSETP/STP 0.960 0.525 0.962 24.011 24.062 0.998 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.033 1.064 0.988 0.959 1.046 0.957ETP7/TP7 BL EBL/BL SED SIN SED/SIN 0.964 1.930 0.980 21.708 21.631 1.004ED12 ED23 ED34 ED45 ED56 ED67 5.966 10.788 2.074 0.109 1.676 1.096 ED45/ED56/ ED67/ ED12/IN12 ED23/IN23 ED34/IN34 IN45 IN56 IN67 0.984 0.9941.094 2.174 0.975 1.045 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.17740.2873 0.2697 0.4043 0.6436 0.1366 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/fIN67/f 0.1597 0.9703 1.1083 0.8755 1.7083 0.2956 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP7 + IN67)/TP6 1.6199 0.9386 4.0321 1.4163 HOS InTL HOS/HOIInS/HOS ODT % TDT % 47.6235 45.6933 9.5247 0.3558 −100.1380 71.9616HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.00000.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.00000.0000 0.0000 0.0000 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.92 0.88 0.850.8 0.72 0.62

The results of the equations of the seventh embodiment based on Table 13and Table 14 are listed in the following table:

Values related to the inflection points of the seventh embodiment(Reference wavelength: 555 nm) HIF111 0 HIF111/HOI 0 SGI111 0 |SGI111|/0 (|SGI111| + TP1)

Eighth Embodiment

As shown in FIG. 8A and FIG. 8B, an optical image capturing system ofthe eighth embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 810, asecond lens 820, a third lens 830, an aperture 800, a fourth lens 840, afifth lens 850, a sixth lens 860, a seventh lens 870, an infrared raysfilter 880, an image plane 890, and an image sensor 892. FIG. 8C shows amodulation transformation of the optical image capturing system 80 ofthe eighth embodiment of the present application in visible spectrum,and FIG.

The first lens 810 has negative refractive power and is made of plastic.An object-side surface 812, which faces the object side, is a convexaspheric surface, and an image-side surface 814, which faces the imageside, is a concave aspheric surface. The object-side surface 812 and theimage-side surface 814 both have an inflection point.

The second lens 820 has negative refractive power and is made ofplastic. An object-side surface 822 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 824thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 822 and the image-side surface 824 both have aninflection point.

The third lens 830 has positive refractive power and is made of plastic.An object-side surface 832, which faces the object side, is a convexaspheric surface, and an image-side surface 834, which faces the imageside, is a convex aspheric surface. The object-side surface 832 andimage-side surface 834 both have an inflection point.

The fourth lens 840 has positive refractive power and is made ofplastic. An object-side surface 842, which faces the object side, is aconvex aspheric surface, and an image-side surface 844, which faces theimage side, is a convex aspheric surface.

The fifth lens 850 has negative refractive power and is made of plastic.An object-side surface 852, which faces the object side, is a concaveaspheric surface, and an image-side surface 854, which faces the imageside, is a concave aspheric surface.

The sixth lens 860 has positive refractive power and is made of plastic.An object-side surface 862, which faces the object side, is a concavesurface, and an image-side surface 864, which faces the image side, is aconvex surface. The object-side surface 862 and the image-side surface864 both have an inflection point. Whereby, the incident angle of eachview field entering the sixth lens 860 can be effectively adjusted toimprove aberration.

The seventh lens 870 has positive refractive power and is made ofplastic. An object-side surface 882, which faces the object side, is aconvex surface, and an image-side surface 884, which faces the imageside, is a concave surface. The image-side surface 874 has an inflectionpoint. It may help to shorten the back focal length to keep small insize. In addition, it may reduce an incident angle of the light of anoff-axis field of view and correct the aberration of the off-axis fieldof view.

The infrared rays filter 880 is made of glass and between the seventhlens 870 and the image plane 890. The infrared rays filter 880 gives nocontribution to the focal length of the system.

The optical image capturing system of the eighth embodiment furthersatisfies ΣPP=76.7754 mm; and f3/ΣPP=0.2346, where ΣPP is a sum of thefocal lengths of each positive lens. It is helpful to share the positiverefractive power of one single lens to other positive lenses to avoidthe significant aberration caused by the incident rays.

The optical image capturing system of the eighth embodiment furthersatisfies ΣNP=−29.9308 mm; and f1/ΣNP=0.4139, where ΣNP is a sum of thefocal lengths of each negative lens. It is helpful to share the negativerefractive power of one single lens to other negative lenses to avoidthe significant aberration caused by the incident rays.

The parameters of the lenses of the eighth embodiment are listed inTable 15 and Table 16.

TABLE 15 f = 3.2022 mm; f/HEP = 2.8; HAF = 70 deg Focal Radius ofThickness Refractive Abbe length Surface curvature (mm) (mm) Materialindex number (mm) 0 Object plane plane 1 1^(st) lens 45.25194153 1.179plastic 1.565 58.00 −13.615 2 6.530553663 2.979 3 2^(nd) lens28.45048651 0.890 plastic 1.565 58.00 −12.389 4 5.567945123 2.258 53^(rd) lens 16.86317406 13.161 plastic 1.550 56.50 18.014 6 −17.490571420.000 7 Aperture plane 0.050 8 4^(th) lens 3.821831971 2.811 plastic1.565 58.00 4.229 9 −4.7192252 0.686 10 5^(th) lens −3.886344092 0.300plastic 1.650 21.40 −3.927 11 7.853851213 0.493 12 6^(th) lens−16.45040823 0.331 plastic 1.607 26.60 35.403 13 −9.416243867 0.050 147^(th) lens 10.04814497 0.521 plastic 1.565 58.00 19.129 15 134.6580461.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 2.99118 Image plane 0.000 plane Reference wavelength (d-line): 555 nm.

TABLE 16 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k4.758702E+00 −5.889217E−02 −6.943469E+00 −5.931587E−02 −1.196153E+01−2.846770E+01 −6.483847E−02 A4 6.227544E−06 −4.117326E−04 −2.236683E−067.492048E−05 −2.173923E−04 8.200135E−04 −2.077686E−04 A6 3.084494E−08−3.728783E−06 −2.602700E−08 −3.594973E−06 −1.336542E−06 2.531078E−041.819755E−05 A8 2.405824E−10 −1.816585E−08 −1.089998E−09 −2.096298E−07−6.065276E−09 −1.249497E−06 −1.055843E−05 A10 1.681390E−12 7.136442E−112.869754E−12 −1.256432E−08 −1.755005E−09 5.139796E−06 −5.651390E−06 A125.933250E−15 1.326333E−12 −4.974101E−12 −6.643498E−10 1.305674E−104.327953E−20 −3.032302E−16 A14 −7.538093E−17 −2.740915E−13 −8.537290E−14−7.544791E−12 −2.655221E−12 8.231837E−25 −7.192269E−24 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k −1.615455E−01 −1.254414E+003.463610E+00 2.303942E+01 −1.893896E+01 −2.877868E+00 5.000000E+01 A4−5.897570E−04 2.278000E−04 5.564271E−04 −4.933293E−04 1.732535E−03−1.952076E−04 5.340317E−04 A6 −1.825644E−04 −6.332738E−04 2.397167E−041.095835E−04 1.847862E−04 5.075190E−06 9.227855E−05 A8 2.019382E−07−1.577314E−04 −8.070753E−06 8.942415E−05 1.970939E−05 6.130407E−061.629776E−05 A10 −5.333494E−06 6.144598E−07 7.661629E−06 1.242952E−055.071654E−06 4.969750E−07 −7.504117E−07 A12 −2.606537E−17 −3.647167E−16−1.006614E−16 −4.105671E−09 2.954683E−09 7.578220E−09 3.011747E−09 A148.064118E−25 −2.699251E−24 2.566758E−22 −5.014763E−22 1.332088E−187.114791E−12 −5.940679E−12 A16 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the eighth embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the eighth embodiment based on Table 15 andTable 16 are listed in the following table:

Eighth embodiment (Reference wavelength: 555 nm) ETP1 ETP2 ETP3 ETP4ETP5 ETP6 1.200 0.914 13.142 2.733 0.363 0.324 ETP7 ETL EBL EIN EIR PIR0.506 29.996 4.289 25.707 0.999 1.000 EIN/ETL SETP/EIN EIR/PIR SETP STPSETP/STP 0.857 0.746 0.999 19.182 19.193 0.999 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.018 1.027 0.999 0.972 1.210 0.979ETP7/TP7 BL EBL/BL SED SIN SED/SIN 0.971 4.291 0.9995 6.524 6.517 1.001ED12 ED23 ED34 ED45 ED56 ED67 2.959 2.238 0.102 0.679 0.462 0.083 ED45/ED56/ ED67/ ED12/IN12 ED23/IN23 ED34/IN34 IN45 IN56 IN67 2.979 2.2580.050 0.686 0.493 0.050 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.23520.2585 0.1778 0.7572 0.8155 0.0905 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/fIN67/f 0.1674 1.1928 1.3092 0.9111 0.9302 0.0156 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP7 + IN67)/TP6 1.0990 0.6877 4.6700 1.7262 HOS InTL HOS/HOIInS/HOS ODT % TDT % 30.0000 25.7092 6.0000 0.3178 −43.1697 27.8256 HVT11HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 1.9821 2.0599 0.0000 0.00000.0000 0.0000 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.89 0.87 0.84 0.770.72 0.59

The results of the equations of the eighth embodiment based on Table 15and Table 16 are listed in the following table:

Values related to the inflection points of the eighth embodiment(Reference wavelength: 555 nm) HIF211 5.4022 HIF211/HOI 1.0804 SGI2110.4801 |SGI211|/(|SGI211| + TP2) 0.3504 HIF221 4.5661 HIF221/HOI 0.9132SGI221 2.1748 |SGI221|/(|SGI221| + TP2) 0.7096 HIF311 3.3316 HIF311/HOI0.6663 SGI311 0.2711 |SGI311|/(|SGI311| + TP3) 0.0202 HIF321 1.3338HIF321/HOI 0.2668 SGI321 −0.0449 |SGI321|/(|SGI321| + TP3) 0.0034 HIF6111.4885 HIF611/HOI 0.2977 SGI611 −0.0694 |SGI611|/(|SGI611| + TP6) 0.1735HIF621 1.3418 HIF621/HOI 0.2684 SGI621 −0.0812 |SGI621|/(|SGI621| + TP6)0.1971

It must be pointed out that the embodiments described above are onlysome embodiments of the present invention. All equivalent structureswhich employ the concepts disclosed in this specification and theappended claims should fall within the scope of the present invention.

What is claimed is:
 1. An optical image capturing system, in order alongan optical axis from an object side to an image side, comprising: afirst lens having refractive power; a second lens having refractivepower; a third lens having refractive power; a fourth lens havingrefractive power; a fifth lens having refractive power; a sixth lenshaving refractive power; a seventh lens having refractive power; and animage plane; wherein the optical image capturing system consists of theseven lenses with refractive power; at least one lens among the firstlens to the seventh lens is made of glass; at least one lens among thefirst lens to the seventh lens is made of plastic; a maximum height forimage formation on the image plane is denoted as HOI; at least one lensamong the first to the seventh lenses has positive refractive power;each lens of the first to the seventh lenses has an object-side surface,which faces the object side, and an image-side surface, which faces theimage side; wherein the optical image capturing system satisfies:1.0≦f/HEP≦10.0;0 deg<HAF≦150 deg; and0.5≦SETP/STP<1; where f1, f2 f3, f4, f5, f6, and f7 are focal lengths ofthe first lens to the seventh lens, respectively; f is a focal length ofthe optical image capturing system; HEP is an entrance pupil diameter ofthe optical image capturing system; HOS is a distance on the opticalaxis between a point on an object-side surface of the first lens wherethe optical axis passes through and a point on the image plane where theoptical axis passes through; InTL is a distance from the object-sidesurface of the first lens to the image-side surface of the seventh lens;HAF is a half of a maximum field angle of the optical image capturingsystem; ETP1, ETP2, ETP3, ETP4, ETP5, ETP6, and ETP7 are respectively athickness at the height of ½ HEP of the first lens, the second lens, thethird lens, the fourth lens, the fifth lens, the sixth lens, and theseventh lens; SETP is a sum of the aforementioned ETP1 to ETP7; TP1,TP2, TP3, TP4, TP5, TP6, and TP7 are respectively a thickness of thefirst lens, the second lens, the third lens, the fourth lens, the fifthlens, the sixth lens, and the seventh lens on the optical axis; STP is asum of the aforementioned TP1 to TP7.
 2. The optical image capturingsystem of claim 1, wherein the optical image capturing system furthersatisfies:0.2≦EIN/ETL<1; where ETL is a distance in parallel with the optical axisbetween a coordinate point at a height of ½ HEP on the object-sidesurface of the first lens and the image plane; EIN is a distance inparallel with the optical axis between the coordinate point at theheight of ½ HEP on the object-side surface of the first lens and acoordinate point at a height of ½ HEP on the image-side surface of theseventh lens.
 3. The optical image capturing system of claim 2, whereinthe optical image capturing system further satisfies:0.3≦SETP/EIN<1.
 4. The optical image capturing system of claim 1,wherein each two neighboring lenses among the first to the seventhlenses are separated by air.
 5. The optical image capturing system ofclaim 1, wherein the image plane is either flat or curved.
 6. Theoptical image capturing system of claim 1, wherein the optical imagecapturing system further satisfies:MTFE0≧0.2;MTFE3≧0.01; andMTFE7≧0.01; where MTFE0, MTFE3, and MTFE7 are respectively a value ofmodulation transfer function of visible light in a spatial frequency of55 cycles/mm at the optical axis, 0.3 HOI, and 0.7 HOI on an imageplane.
 7. The optical image capturing system of claim 1, furthercomprising a filtering component provided between the seventh lens andthe image plane, wherein the optical image capturing system furthersatisfies:0.1≦EIR/PIR≦1.1; where DR is a horizontal distance in parallel with theoptical axis between the coordinate point at the height of ½ HEP on theimage-side surface of the seventh lens and the filtering component; PIRis a horizontal distance in parallel with the optical axis between apoint on the image-side surface of the seventh lens where the opticalaxis passes through and the filtering component.
 8. The optical imagecapturing system of claim 1, wherein the optical image capturing systemfurther satisfies:0.1≦EBL/BL≦1.1; where EBL is a horizontal distance in parallel with theoptical axis between a coordinate point at the height of ½ HEP on theimage-side surface of the seventh lens and image surface; BL is ahorizontal distance in parallel with the optical axis between the pointon the image-side surface of the seventh lens where the optical axispasses through and the image plane.
 9. The optical image capturingsystem of claim 1, further comprising an aperture and an image sensor,wherein the image sensor is provided on the image plane; the opticalimage capturing system further satisfies:0.1≦InS/HOS≦1.1; and0≦HIF/HOI≦0.9; where InS is a distance on the optical axis between theaperture and the image plane.
 10. An optical image capturing system, inorder along an optical axis from an object side to an image side,comprising: a first lens having negative refractive power; a second lenshaving refractive power; a third lens having refractive power; a fourthlens having refractive power; a fifth lens having refractive power; asixth lens having refractive power; a seventh lens having refractivepower; and an image plane; wherein the optical image capturing systemconsists of the seven lenses with refractive power; the first lens ismade of glass, and at least two lenses among the second lens to theseventh lens are made of plastic; a maximum height for image formationon the image plane is denoted as HOI; each lens among the first to theseventh lenses has an object-side surface, which faces the object side,and an image-side surface, which faces the image side; at least one lensamong the second lens to the seventh lens has positive refractive power;wherein the optical image capturing system satisfies:1.0≦f/HEP≦10.0;0 deg<HAF≦150; and0.2≦EIN/ETL<1; where f1, f2 f3, f4, f5, f6, and f7 are focal lengths ofthe first lens to the seventh lens, respectively; f is a focal length ofthe optical image capturing system; HEP is an entrance pupil diameter ofthe optical image capturing system; HOS is a distance on the opticalaxis between a point on an object-side surface of the first lens wherethe optical axis passes through and a point on the image plane where theoptical axis passes through; InTL is a distance from the object-sidesurface of the first lens to the image-side surface of the seventh lens;HAF is a half of the maximum field angle of the optical image capturingsystem; ETL is a distance in parallel with the optical axis between acoordinate point at a height of ½ HEP on the object-side surface of thefirst lens and the image plane; EIN is a distance in parallel with theoptical axis between the coordinate point at the height of ½ HEP on theobject-side surface of the first lens and a coordinate point at a heightof ½ HEP on the image-side surface of the seventh lens.
 11. The opticalimage capturing system of claim 10, wherein the optical image capturingsystem further satisfies:0<ED67/IN67≦50; where ED67 is a horizontal distance between the sixthlens and the seventh lens at the height of ½ HEP; IN67 is a horizontaldistance between the sixth lens and the seventh lens on the opticalaxis.
 12. The optical image capturing system of claim 10, wherein theoptical image capturing system further satisfies:0<ED12/IN12≦35; where ED12 is a horizontal distance between the firstlens and the second lens at the height of ½ HEP; IN12 is a horizontaldistance between the first lens and the second lens on the optical axis.13. The optical image capturing system of claim 10, wherein each twoneighboring lenses among the first to the seventh lenses are separatedby air.
 14. The optical image capturing system of claim 10, wherein theoptical image capturing system further satisfies:0<ETP6/TP6≦3; where ETP6 is a thickness of the sixth lens at the heightof ½ HEP in parallel with the optical axis; TP6 is a thickness of thesixth lens on the optical axis.
 15. The optical image capturing systemof claim 10, wherein the optical image capturing system furthersatisfies:0<ETP7/TP7≦5; where ETP7 is a thickness of the seventh lens at theheight of ½ HEP in parallel with the optical axis; TP7 is a thickness ofthe seventh lens on the optical axis.
 16. The optical image capturingsystem of claim 10, wherein the optical image capturing system furthersatisfies:0<IN12/f≦60; where IN12 is a distance on the optical axis between thefirst lens and the second lens.
 17. The optical image capturing systemof claim 10, wherein the optical image capturing system furthersatisfies:MTFI0≧0.01;MTFI3≧0.01; andMTFI7≧0.01; where MTFI0, MTFI3, and MTFI7 are respectively values ofmodulation transfer function for an infrared of wavelength of 850 nm ina spatial frequency of 55 cycles/mm at the optical axis, 0.3 HOI, and0.7 HOI on the image plane.
 18. The optical image capturing system ofclaim 10, wherein the optical image capturing system further satisfies:MTFQ0≧0.2;MTFQ3≧0.01; andMTFQ7≧0.01 where HOI is a maximum height for image formationperpendicular to the optical axis on the image plane; MTFQ0, MTFQ3, andMTFQ7 are respectively values of modulation transfer function of visiblelight in a spatial frequency of 110 cycles/mm at the optical axis, 0.3HOI, and 0.7 HOI on the image plane.
 19. The optical image capturingsystem of claim 10, wherein at least one lens among the first lens tothe seventh lens is a light filter, which is capable of filtering outlight of wavelengths shorter than 500 nm.
 20. An optical image capturingsystem, in order along an optical axis from an object side to an imageside, comprising: a first lens having negative refractive power; asecond lens having refractive power; a third lens having refractivepower; a fourth lens having refractive power; a fifth lens havingrefractive power; a sixth lens having refractive power; a seventh lenshaving refractive power; and an image plane; wherein the optical imagecapturing system consists of the seven lenses having refractive power;two lenses among the first lens to the seventh lens are made of plastic,while the other five lenses are made of glass; at least one lens amongthe second to the fourth lens has positive refractive power; at leastone lens among the fifth lens to the seventh lens has positiverefractive power; the a maximum height for image formation on the imageplane is denoted as HOI; each lens of the first to the seventh lenseshas an object-side surface, which faces the object side, and animage-side surface, which faces the image side; the object-side surfaceor the image-side surface of each of at least one lens among the firstlens to the seventh lens has at least an inflection point; wherein theoptical image capturing system satisfies:1.0≦f/HEP≦10;0 deg<HAF≦100; and0.2≦EIN/ETL<1; where f1, f2 f3, f4, f5, f6, and f7 are focal lengths ofthe first lens to the seventh lens, respectively; f is a focal length ofthe optical image capturing system; HEP is an entrance pupil diameter ofthe optical image capturing system; HOS is a distance on the opticalaxis between a point on an object-side surface of the first lens wherethe optical axis passes through and a point on the image plane where theoptical axis passes through; InTL is a distance from the object-sidesurface of the first lens to the image-side surface of the seventh lenson the optical axis; HAF is a half of a maximum field angle of theoptical image capturing system; ETL is a distance in parallel with theoptical axis between a coordinate point at a height of ½ HEP on theobject-side surface of the first lens and the image plane; EIN is adistance in parallel with the optical axis between the coordinate pointat the height of ½ HEP on the object-side surface of the first lens anda coordinate point at a height of ½ HEP on the image-side surface of theseventh lens.
 21. The optical image capturing system of claim 20,wherein each two neighboring lenses among the first to the seventhlenses are separated by air.
 22. The optical image capturing system ofclaim 21, wherein the optical image capturing system further satisfies:0.1≦EBL/BL≦1.1; where EBL is a horizontal distance in parallel with theoptical axis between a coordinate point at the height of ½ HEP on theimage-side surface of the seventh lens and image surface; BL is ahorizontal distance in parallel with the optical axis between the pointon the image-side surface of the seventh lens where the optical axispasses through and the image plane.
 23. The optical image capturingsystem of claim 20, wherein the optical image capturing system furthersatisfies:0<ED67/IN67≦50; where ED67 is a horizontal distance between the sixthlens and the seventh lens at the height of ½ HEP; IN67 is a horizontaldistance between the sixth lens and the seventh lens on the opticalaxis.
 24. The optical image capturing system of claim 23, wherein theoptical image capturing system further satisfies:0<IN67/f≦5.0; where IN67 is a horizontal distance between the sixth lensand the seventh lens on the optical axis.
 25. The optical imagecapturing system of claim 23, further comprising an aperture, an imagesensor, and a driving module, wherein the image sensor is disposed onthe image plane; the driving module is coupled with the lenses to movethe lenses; the optical image capturing system further satisfies:0.1≦InS/HOS≦1.1; where InS is a distance on the optical axis between theaperture and the image plane.